{ "version": "mdr-organic-filtered-export/1.0.0", "source_snapshot_sha256": "5da57e0959d1ea0c081460dbf24a62b2eacfcb0d179ad1bfcbc272bdfd2ea3bd", "filters": { "q": "", "structure": "", "field": "", "row": "" }, "matches": 568, "scope": "all_matching_source_rows_not_only_the_visible_page", "source_dataset": { "version": "mdr-organic-reference/1.0.0", "dataset_version": "240322", "dataset_url": "https://doi.org/10.48505/nims.4487", "source": { "filename": "240322_MDR_Organic.txt", "bytes": 263372, "sha256": "d116848a90d01e48356ed6cf0bb69035fa863a3a559deac1ef188025bdb3b423", "header_sha256": "c1e031a258d9c822eeba109fb40a76198219af1735c35c586f7332dbaf936fa7", "url": "https://mdr.nims.go.jp/filesets/1a18e447-8ec2-4316-be12-b4acdc885fb8/download", "guide_url": "https://mdr.nims.go.jp/filesets/dd00e931-e7b7-4bc5-bde2-ba0ff1e9adaf/download", "guide_page": 9, "guide_sha256": "89096c1f006a5d5c256d14394880b31684ad2ce0b4f7ea0d37175256ea6a029d" }, "attribution": "MDR SuperCon Datasheet Ver.240322, National Institute for Materials Science (NIMS), DOI 10.48505/nims.4487. SCLib preserves all original Organic cells and adds row provenance and a reading interface.", "license": "CC BY 4.0", "license_url": "https://creativecommons.org/licenses/by/4.0/", "columns": [ "num", "refno", "name", "fullname", "shape", "str", "lata", "latb", "latc", "alpha", "beta", "lgamma", "tc", "tcmax", "pmax", "pcrit", "tcmeth", "isotope", "isoel", "dtcdp", "tcn", "hc1zero", "hc2zero", "dhc2dt", "cohere", "penet", "glpar", "gap", "gapmeth", "gamma", "debyet", "curiet", "neelt", "fig1", "fig2", "figname", "tbl", "tblname", "commt", "f1_filename", "f2_filename", "title", "year", "keyword", "institute", "journal", "author", "sample", "comments" ], "source_labels": [ "data number", "reference number", "common formula of materials", "full material name", "shape", "structure", "lattice constant a", "lattice constant b", "lattice constant c", "lattice alpha", "lattice beta", "lattice gamma", "Tc at pcrit or Tc at atmospheric pressure", "maximum tc under pressure", "applied pressure for tcmax", "Critical pressure/GPa at which Tc can be observed", "tc measurement method", "alpha in Tc=A*M^(-alpha), isotope effect", "isotope element", "slope at P=0 in Tc vs P plot ", "lowest temperature for measurement (not superconducting)", "Hc1 at 0 K for poly crystal", "Hc2 at 0 K for poly crystal", "-slope in Hc2 vs T at Tc for poly crystal", "coherence length at 0 K for poly crystal", "penetration depth at 0 K for poly crystal", "Ginzburg-Landau order parameter", "energy gap at 0 K, delta(0)", "method of measuring energy gap", "coefficient of electronic specific heat", "Debye temperature", "Curie temperature", "Neel temperature", "figure1 file name", "figure2 filename", "figure description", "table file name", "table description", "comment", "figure1 data file name", "f2 data file name", "title", "year", "keyword", "institute", "journal", "author", "sample", "comments" ], "excluded_rows": [ { "line_start": 571, "line_end": 571, "sha256": "bdcb2dde8c9d958f2a70c6621f26b4f099b6057b28f63d7480f0401130ebdd9e", "reason": "all_cells_empty" } ], "coverage": { "num": 568, "refno": 568, "name": 563, "fullname": 568, "shape": 234, "str": 566, "lata": 109, "latb": 107, "latc": 109, "alpha": 42, "beta": 84, "lgamma": 42, "tc": 517, "tcmax": 83, "pmax": 74, "pcrit": 484, "tcmeth": 39, "isotope": 28, "isoel": 52, "dtcdp": 53, "tcn": 23, "hc1zero": 21, "hc2zero": 70, "dhc2dt": 37, "cohere": 73, "penet": 41, "glpar": 10, "gap": 15, "gapmeth": 9, "gamma": 31, "debyet": 24, "curiet": 10, "neelt": 20, "fig1": 162, "fig2": 22, "figname": 5, "tbl": 1, "tblname": 0, "commt": 527, "f1_filename": 157, "f2_filename": 21, "title": 557, "year": 568, "keyword": 21, "institute": 328, "journal": 568, "author": 567, "sample": 26, "comments": 1 }, "interpretation": { "units": "Only pcrit explicitly names GPa in the table header. Other numeric columns have no unit columns; no numeric normalization is performed.", "tc": "The actual source header says Tc at pcrit or atmospheric pressure; the guide abbreviates it as Tc at pcrit. Missing pcrit does not establish ambient pressure.", "tcmax": "Maximum Tc under pressure; pmax is its associated applied pressure, unlike the oxide/metallic table pmax definition.", "tcn": "Lowest measurement temperature for a non-superconducting report, not a Tc value.", "names": "Common name can contain only the counterion; full name, structure label, isotope and comments remain separate. No molecular expansion, phase or sample matching is inferred." }, "scope": { "source_publication_status": "not_checked", "scientific_acceptance": false, "catalogue_association": "unestablished", "ml_training_approved": false, "canonical_properties_modified": false } }, "rows": [ { "id": "1", "line_start": 3, "line_end": 3, "sha256": "cf3fefca095b1a64b78a0acb4c7e67d1eb41d674a821630b4b374c4cca485349", "values": [ "1", "PR05403760", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "", "", "", "", "", "", "", "9.5", "", "", "0", "2", "", "", "", "", "", "5.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "magnetization, Hc2, Hirr", "", "", "Anomalous magnetization and dimensional crossover of the vortex system in the organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "1996", "", "Institute for Materials Research, Tohoku University, Sendai 980-77, Japan", "Phys.Rev.B, 54(1996)3760", "N.Kobayashi,T.Fukase,T.Nishizaki,T.Sasaki", "", "" ] }, { "id": "2", "line_start": 4, "line_end": 4, "sha256": "625322634e39c58982bfd77e726192d149e291824bd0ba19432ef064afea1ac4", "values": [ "2", "JPS0652987", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "2", "BEDT-TTF", "", "", "", "", "", "", "12.6", "12.6", "0.03", "0.03", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "hydrogenated BEDT-TTF. Tc(M to S)=12.6 K and Tc(S to M)=6.7 at P=0.03 GPa. Tc is nearly independent of P. Re-entrant.", "", "", "Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure", "1996", "", "Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 65(1996)2987", "H.Ito,T.Ishiguro,M.Kubota,G.Saito", "", "" ] }, { "id": "3", "line_start": 5, "line_end": 5, "sha256": "254f7b03da05ea92d61bea2468b85c32b00989eb593a91c6f63cd2c73a20b19b", "values": [ "3", "JPS0652987", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "2", "BEDT-TTF", "", "", "", "", "", "", "13", "13", "0.045", "0.044", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "deuterated BEDT-TTF. Tc(M to S)=13.0 K and Tc(S to M)=7.2 at P=0.05 GPa. Tc is nearly independent of P. Re-entrant.", "", "", "Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure", "1996", "", "Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 65(1996)2987", "H.Ito,T.Ishiguro,M.Kubota,G.Saito", "", "" ] }, { "id": "4", "line_start": 6, "line_end": 6, "sha256": "870090a1d4fc5f1541f849b332efad5abd89e37f325f3c29acc486056d026c91", "values": [ "4", "PR05705610", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11.5", "", "", "0", "1", "", "", "", "", "", "8", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "R has a peak at Tc(on). This peak corresponds to Hc2. Value of Hc2zero is at T=2 K..", "", "", "Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br", "1998", "", "Department of Physics, University of Miami, Coral Gables, florida 33124", "Phys.Rev.B,57(1998)R5610-R5613", "F. Zuo,F.Zuo,J.A. Schlueter,J.A.Schlueter,J.M.Williams,Jack M. Williams,M.E. Kelly,M.E.Kelly,P. Zhang,P.Zhang,X. Su,X.Su", "", "" ] }, { "id": "5", "line_start": 7, "line_end": 7, "sha256": "b016d81c5539911a41079f6ba6e4e44fd015dff0d81100ed7ce80e0dfb680229", "values": [ "5", "PR05703623", "NH4Hg(SCN)4", "alpha-(BEDT-TTF)2NH4Hg(SCN)4", "2", "BEDT-TTF", "", "", "", "", "", "", "0.95", "", "", "0", "2", "", "", "", "", "", "", "0.08", "500", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "Hc2 by sp-heat and M-H. out-of-plane PENET(by SUS) = 1400 um. Anisotropy factor = 2000. interlayer spacing = 20 A.", "", "", "Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy", "1998", "", "Institute for Molecular Science, Myodaiji, Okazaki 444, Japan", "Phys.Rev.B,57(1998)3623", "H.Taniguchi,Hiromi Taniguchi,K.Kanoda,Kazushi Kanoda,Y.Nakazawa,Yasuhiro Nakazawa", "", "" ] }, { "id": "6", "line_start": 8, "line_end": 8, "sha256": "99d432c2036531554e978b78553d7c0af152698b284e237bb28aefb6e83c7c2e", "values": [ "6", "PR04915227", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.14", "", "", "0", "", "", "", "", "", "", "", "1.3", "53", "", "", "", "", "", "", "", "", "", "", "", "", "", "dHc2/dT]//ab = 13 T/K. cohere//c = 5.2 A. anisotropy factor = 100. Hc2, Hirr were measured.", "", "", "Fluctuation effects and mixed-state properties of the layered organic superconductors k-(BEDT-TTF)2Cu(NCS)2 and k-(BEDT-TTF)2Cu[N(CN)2]Br", "1994", "", "", "Phys.Rev.B, 49(1994)15227", "F.Steglich,M.Lang,N.Toyota,T.Sasaki", "organic", "" ] }, { "id": "7", "line_start": 9, "line_end": 9, "sha256": "eb20d94622fda0d09aa8102a729e22e92132caedfffb4267b483b531a9861818", "values": [ "7", "PR04915227", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11.4", "", "", "0", "", "", "", "", "", "", "", "3.8", "28", "", "", "", "", "", "", "", "", "", "", "", "", "", "dHc2/dT]//ab = 21 T/K. cohere//c = 4.9 A. Hc2, anisotropy factor = 30. Hirr were measured.", "", "", "Fluctuation effects and mixed-state properties of the layered organic superconductors k-(BEDT-TTF)2Cu(NCS)2 and k-(BEDT-TTF)2Cu[N(CN)2]Br", "1994", "", "", "Phys.Rev.B, 49(1994)15227", "F.Steglich,M.Lang,N.Toyota,T.Sasaki", "organic", "" ] }, { "id": "8", "line_start": 10, "line_end": 10, "sha256": "dce49e41b70f99480080c3a8e87b1ef0fcd35dc4698f08646573e01592156d87", "values": [ "8", "JPS0720468", "ICl2", "beta'-(BEDT-TTF)2ICl2", "2", "BEDT-TTF", "", "", "", "", "", "", "14.2", "14.2", "8.2", "7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "22", "", "", "", "", "", "Neel-T from Synth.Met. 86(1997)2029. Structure is modified beta-type.", "", "", "Superconductivity at 14.2K in Layered Organics under Extreme Pressure", "2003", "", "Department of Physics, Faculty of Science, Saitama University, Shimo-Ohkubo 255, Saitama, Japan", "J.Phys.Soc.Jpn, 72(2003)468", "H.Okamoto,H.Taniguchi,K.Kanoda,K.Miyagawa,K.Satoh,K.Uchiyama,M.Hedo,M.Miyashita,N.Mori,Y.Uwatoko", "", "" ] }, { "id": "9", "line_start": 11, "line_end": 11, "sha256": "562000bc998fd64744053ec0fdfbb589889d4be6af19d6835d56f2d4b18bf86f", "values": [ "9", "JPS0712240", "NH4Hg(SCN)4", "alpha-(BEDT-TTF)2NH4Hg(SCN)4", "2", "BEDT-TTF", "", "", "", "", "", "", "1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "hexagonal shaped crystal. Tc(on) = 2.0 K. Sp-heat, thermal-C, AC-sus, were measured in H//plane.", "", "", "Superconducting State of the Layered Conductor alpha-(BEDT-TTF)2NH4Hg(SCN)4 in Magnetic Fields Parallel to the Layer Plane", "2002", "", "Physics Department, Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 71(2002)2240", "A.E.Kovalev,G.Saito,H.Yamochi,M.A.Tanatar,T.Ishiguro,Y.Shimojo", "", "" ] }, { "id": "10", "line_start": 12, "line_end": 12, "sha256": "ddbb93ab65e0b1edd90bfcf2fa0556e5a81277711711b72ab263d7058991d6c4", "values": [ "10", "JPS0711716", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "2", "BEDT-TTF", "", "", "", "", "", "", "7", "7", "0.19", "0.03", "", "", "", "", "", "", "2", "", "130", "", "", "", "", "", "", "", "", "", "", "", "", "", "values are at P=1.9 kbar. Tc(P=1.9 kbar) = 7. K. Hc2(0)//ab = 18 T, cohere//c = 13 A.", "", "", "Upper Critical Field of kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Magnetic Fields Parallel to the Superconducting Plane", "2002", "", "Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 71(2002)1716", "G.Saito,H.Yamochi,T.Ishiguro,Y.Shimojo", "", "" ] }, { "id": "11", "line_start": 13, "line_end": 13, "sha256": "7a85629b3ab19afb2b87a074da2346fef10122e644f11e245dcf6a8e5a9e6929", "values": [ "11", "PR04404666", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "2", "BEDT-TTF", "", "", "", "", "", "", "12.8", "12.8", "0.03", "0.03", "", "", "", "-32", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope effect(H-D) shows inverse effect (See Fig).", "", "", "Pressure-temperature phase diagram, inverse isotope effect, and superconductivity in excess of 13 K in kappa-(BEDT-TTF)2Cu[N(CN)2]Cl, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene", "1991", "", "Sandia National Laboratories, Albuquerque, New Mexico,USA", "Phys.Rev.B, 44(1991)4666", "A.M.Kini,B.J.Love,D.L.Overmyer,D.M.Watkins,G.A.Yaconi,H.A.Charlier,H.Hau Wang,J.E.Schirber,J.M.Williams,K.D.Carlson", "", "" ] }, { "id": "12", "line_start": 14, "line_end": 14, "sha256": "e8382bccfe2503a7ecb7b574bd8631c0d16faab97f23a3b92346237cfbb7bda2", "values": [ "12", "PHC1520157", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "-30", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "EFFEDT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF K(BEDT-TTF)2CU(NCS)2", "1988", "", "", "PHYSICA C,152(1988)157", "A.M.Kini,E.L.Venturini,H.H.Wang,J.E.Schirber,J.M.Williams,J.R.Ehitworth,KINI.A.M,SCHIRBER.J.E,VENTURINI.E.L,WANG.H.H,WHITWORTH.J.R,WILLIAMS.J.M", "", "" ] }, { "id": "13", "line_start": 15, "line_end": 15, "sha256": "5bbb74b7adb2f4ed6b342ef8badc997798cd75999e5605c51b75fa8a442f8a61", "values": [ "13", "PHC1700231", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "-24", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "PRESSURE DEPENDENCE OF TC IN THE HIGHEST TC ORGANIC SUPERCONDUCTOR K-(BEDT-TTF)2CU(N(CN)2) BR", "1990", "", "SANDIA NATIONAL LABORATORIES, ALBUQUERQUE, NM 87185, USA", "PHYSICA C,170(1990)231", "A.M.KINI,A.M.Kini,D.L.OVERMYER,D.L.Overmyer,H.H.WAMG,H.H.Wang,J.E.SCHIRBER,J.E.Schirber,J.M.WILLIAMS,J.M.Williams", "", "" ] }, { "id": "14", "line_start": 16, "line_end": 16, "sha256": "6abecd17efb1fadaaf5d079382d1691cca88395c0e75305adb3d497770b32a49", "values": [ "14", "PHC4000059", "ClO4", "(TMTSF)2ClO4", "", "TMTSF", "", "", "", "", "", "", "1.15", "", "", "0", "", "", "", "", "", "", "", "", "", "1.23", "", "", "", "", "", "", "", "", "", "", "", "", "Tc and lamda are obtained by fitting of muon-SR data.", "", "", "Muon spin rotation study of the (TMTSF)2ClO4 system", "2003", "", "Department of Physics, Gonzaga University, 502 E. Boone Avenue, Spokane, WA 99258-0051, USA", "Physica C, 400(2003)59", "A.Goonewardene,A.J.Greer,D.Ll.Williams,D.R.Harshman,E.Koster,R.C.Haddon,R.N.Kleiman,W.J.Kossler,W.Kang", "", "" ] }, { "id": "15", "line_start": 17, "line_end": 17, "sha256": "99a89921bccc4eb9fe21bd6260eec8190fe33ae58ad807f752ba3ea559fe1b3d", "values": [ "15", "P067174511", "SbF6", "beta-(BDA-TTP)2SbF6", "", "BDA-TTP", "", "", "", "", "", "", "6.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "33", "", "", "", "", "", "", "", "", "delta-C/gamma*Tc = 1.1. dHvA effect measured.", "", "", "Fermiology and superconductivity studies on the non-tetrachalcogenafulvalene-structured organic superconductor beta-(BDA-TTP)2SbF6", "2003", "", "National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida,USA", "Phys.Rev.B, 67(2003)174511", "A.Wade,E.Goetz,E.Jobilong,E.S.Choi,J.S.Brooks,J.Yamada,M.Tokumoto,T.Kinoshita,T.Mizutani", "", "" ] }, { "id": "16", "line_start": 18, "line_end": 18, "sha256": "2a9d23ab48ec3eb40e2ddd24771d105ef4b8fba04e4ac9f2be968dc6bfeed6a0", "values": [ "16", "PHC3310292", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.5", "", "", "0", "", "", "", "", "", "", "11.3", "1.6", "54", "0.48", "71", "", "", "", "", "", "", "", "", "", "", "", "Hc2 calculated based on magnetization curves.", "", "", "Magnetization study of organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2000", "", "National Creative Research Initiative Center for Superconductivity, Department of Physics, Pohang University of Science and Technology, Pohang, Kyungbuk 790-784, South Korea", "Physica C,331(2000)292-296", "H-J.Kim,Hyeong-Jin Kim,Jae-Hyuk Choi,Jin-Tae Kim,Mun-Seog Kim,Sung-Ik Lee", "", "" ] }, { "id": "17", "line_start": 19, "line_end": 19, "sha256": "69174a80ea126fa9eec2e6b8bebcc858ae367df18f8f59499f8415398d5c431d", "values": [ "17", "P063104518", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "10.4", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "6.7", "1", "", "", "", "", "", "", "", "", "", "gap in b-c plane.", "", "", "Tunneling spectroscopy on the organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 using STM", "2001", "", "Division of Physics, Hokkaido University, Sapporo 060-0810, Japan", "Phys.Rev.B, 63(2001)104518", "H.Anzai,J.Yamada,K.Ichimura,K.Nomura,S.Nakatsuji,S.Takasaki,T.Arai", "", "" ] }, { "id": "18", "line_start": 20, "line_end": 20, "sha256": "088a690cd2a9058f4550759f53c8fbd443922d30d1d84a52fce4f3771a4ce1d9", "values": [ "18", "P065140508", "AuI2", "(MDT-TSF)(AuI2)0.44", "2", "MDT-TSF", "4.016", "", "12.513", "", "", "", "4.5", "", "", "0", "", "", "", "", "", "", "", "", "262", "", "", "", "", "", "300", "", "", "OHC18", "", "", "", "", "incommensurate chain structure. cohere< b >=100 A. cohere< c >=50 A.", "OHC18.dat", "", "Organic superconductor with an incommensurate anion structure: (MDT-TSF)(AuI2)0.44", "2002", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan", "Phys.Rev.B, 65(2002)140508", "K.Takimiya,T.Kawamoto,T.Mori,T.Otsubo,Y.Aso,Y.Kataoka", "", "" ] }, { "id": "19", "line_start": 21, "line_end": 21, "sha256": "9c22b518730bbaaeecc671a3d94b95caa5041a8d55c30aeac1d89cda28e1197c", "values": [ "19", "P065064516", "Cu[N(CN)2]I", "kappa-(BEDT-TTF)2Cu[N(CN)2]I", "2", "BEDT-TTF", "", "", "", "", "", "", "7.7", "7.7", "0.12", "0.12", "", "", "", "-17", "1.2", "", "", "5.45", "113", "", "", "", "", "", "", "", "", "OHC19", "", "", "", "", "conducting plane = ac-plane. SC properties are at P=0.12 GPa. For H//b, cohere(b) = 8 A, (dHc2/dT) = 0.38 T/K at Tc.", "OHC19.dat", "", "Pressure-temperature phase diagram of the organic superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]I", "2002", "", "Department of Physics, Kyoto University, Kyoto 606-8502, Japan", "Phys.Rev.B, 65(2002)64516", "E.B.Yagubskii,M.A.Tanatar,N.D.Kushch,S.Kagoshima,T.Ishiguro", "", "" ] }, { "id": "20", "line_start": 22, "line_end": 22, "sha256": "ae462aefcb52a5313a18e1e60d60d571d52324f685bc92f99209b79d5b9f378b", "values": [ "20", "JPS0721014", "Au(CN)4", "theta-(DIETS)2[Au(CN)4]", "3", "DIETS", "", "", "", "", "", "", "8.6", "8.6", "1", "0.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not s/c for a- and b-uniaxial pressure. s/c only for c-axial pressure. M-I transition temperature decreases linearly with increasing P(c-axis). T = 14 K at P(c-axis) = 6.5 kbar.", "", "", "Uniaxial Strain Effects on Transport Properties of a Supramolecular Organic Conductor theta-(DIETS)2[Au(CN)4]", "2003", "", "Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama, Japan", "J.Phys.Soc.Jpn, 72(2003)1014", "K.Kajita,N.Tajima,R.Kato,T.Imakubo,Y.Nishino", "", "" ] }, { "id": "21", "line_start": 23, "line_end": 23, "sha256": "ca99f49949ee4630602cd97dd98d2ffef668cdb5271f364018ab2eae0a18e31c", "values": [ "21", "JPS0711832", "I3", "alpha-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "7", "7", "0.2", "0.15", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not s/c for hydrostatic pressure. s/c only for a-axial pressure. M-I phase transition at 135 K under P = 0.", "", "", "Effects of Uniaxial Strain on Transport Properties of Organic Conductor alpha-(BEDT-TTF)2I3 and Discovery of Superconductivity", "2002", "", "Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama, Japan", "J.Phys.Soc.Jpn, 71(2002)1832", "A.Ebina-Tajima,K.Kajita,M.Tamura,N.Tajima,Y.Nishio", "", "" ] }, { "id": "22", "line_start": 24, "line_end": 24, "sha256": "8219bb7bc89b685d4d5b1f8a7bf513bfb0de68a7f35d137b9ee4d860ff8a3469", "values": [ "22", "P066134503", "GaCl4", "Lamda-(BETS)2GaCl4", "2", "BETS", "", "", "", "", "", "", "5.6", "", "", "0", "1", "", "", "", "", "", "", "4.3", "116", "", "", "", "", "", "", "", "", "", "", "", "", "", "Hc2 determined from RES(mid) and thermal conductivity. dHc2/dT for //c = 0.45 T/K. cohere = 12 A. RRR=20.", "", "", "Magnetic field-temperature phase diagram of the quasi-two-dimensional organic superconductor lamda-(BETS)2GaCl4 studied via thermal conductivity", "2002", "", "Department of Physics, Kyoto University, Kyoto 606-8502, Japan", "Phys.Rev.B, 66(2002)134503", "H.Kobayashi,H.Tanaka,M.A.Tanatar,T.Ishiguro", "", "" ] }, { "id": "23", "line_start": 25, "line_end": 25, "sha256": "a659fbc074448d9cf4151cb20824232ad6e6318d7bb29979fb578578e26e67e6", "values": [ "23", "EPJ0250319", "PF6", "(TMTSF)2PF6", "2", "TMTSF", "", "", "", "", "", "", "1.21", "1.21", "0.89", "0.865", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SDW-region for 0 - 0.93 GPa. T(P=0) = 10.2 K.", "", "", "Coexistence of superconductivity and spin density wave orderings in the organic superconductor (TMTSF)2PF6", "2002", "", "Universite Paris-Sud, Orsay, France", "Eur.Phys.J.B, 25(2002)319", "C.Pasquier,D.Jerome,K.Bechgaard,M.Heritier,P.Auban-Senzier,S.Tomic,T.Vuletic", "", "" ] }, { "id": "24", "line_start": 26, "line_end": 26, "sha256": "01cf2a9f935d15c6921d96bbc21c8ab93d43fe5dc5c6f6458368faa2c8a29fe3", "values": [ "24", "JPS0710717", "SbF6", "beta-(BDA-TTF)2SbF6", "2", "BDA-TTF", "", "", "", "", "", "", "6.31", "", "", "0", "1", "", "", "", "", "0.5", "12", "", "105", "0.68", "260", "", "", "", "", "", "", "", "", "", "", "", "Hc1(0)//c = 1.5 mT. Hc2(0)//c = 3 T. cohere< c > =26 A. penet< c > = 0.27 micron. G-L< c > = 60.", "", "", "Superconductivity of Layered Organic Compound beta-(BDA-TTP)2SbF6, Where BDA-TTP is 2,5-Bis(1,3-dithian-2-ylidene)-1,3,4,6-tetrathiapentalene", "2002", "", "Physics Department, Kyoto University, Kyoto 606-8", "J.Phys.Soc.Jpn, 71(2002)717", "J.Yamada,T.Ishiguro,T.Toita,Y.Shimojo", "", "" ] }, { "id": "25", "line_start": 27, "line_end": 27, "sha256": "20b75551fc0d937c7282d2dd50786210ee2a845dd63229226794a5f38d494994", "values": [ "25", "PRL0691443", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.15", "", "", "0", "", "", "", "", "", "", "", "", "", "0.62", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Magnetic penetration depth of kappa-(BEDT-TTF)2Cu(NCS)2: Strong evidence for conventional Cooper pairing", "1992", "", "Institute for Materials Research, Tohoku University, Sendai, Japan", "Phys.Rev.Lett., 69(1992)1443", "H.Sato,M.Lang,N.Toyota,T.Sasaki", "", "" ] }, { "id": "26", "line_start": 28, "line_end": 28, "sha256": "e7066afc2500a488af7f8d6a5490b8e6d19245c8b7ec42b024647569056bbfa0", "values": [ "26", "P064214517", "BF4", "(TMET-STF)2BF4", "2", "TMET-STF", "", "", "", "", "", "", "4.1", "", "", "0", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "cohere(T) for H//ab and H//c were calculated from Hc2(T).", "", "", "Anisotropic superconductivity and dimensional crossover in (TMET-STF)2BF4", "2001", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 64(2001)214517", "C.Terakura,R.Kato,S.Uji,T.Terashima,Y.Okano", "", "" ] }, { "id": "27", "line_start": 29, "line_end": 29, "sha256": "0023d4ec82a94ce7bbaafc2df68603fad2d564f79f175984bcdeea254e47b295", "values": [ "27", "PR05508670", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.06", "212", "", "", "", "", "", "", "", "substitution of all 8 H atoms with D.", "", "", "Low-temperature specific heat of k-(BEDT-TTF)2Cu[N(CN)2]Br in the superconducting state", "1997", "", "Institute for Molecular Science, Myodaiji, Okazaki 444, Japan", "Phys.Rev.B,55(1997)R8670", "K. Kanoda,K.Kanoda,Y. Nakazawa,Y.Nakazawa", "", "" ] }, { "id": "28", "line_start": 30, "line_end": 30, "sha256": "2c973451c497b5af52f8215c3e9573750434d80e02937e859577b6204c8a1f25", "values": [ "28", "PR05508670", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "12", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "213.7", "", "", "", "", "", "", "", "hydrated. h8-BEDT-TTF", "", "", "Low-temperature specific heat of k-(BEDT-TTF)2Cu[N(CN)2]Br in the superconducting state", "1997", "", "Institute for Molecular Science, Myodaiji, Okazaki 444, Japan", "Phys.Rev.B,55(1997)R8670", "K. Kanoda,K.Kanoda,Y. Nakazawa,Y.Nakazawa", "", "" ] }, { "id": "29", "line_start": 31, "line_end": 31, "sha256": "101626100185abe7a7ea6dd392e0806e82eec78c2887b2108abbdaf1d79d9e59", "values": [ "29", "PHC2590181", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9", "", "", "0", "", "", "", "", "", "", "", "", "81", "0.6", "74", "", "", "", "", "", "", "", "", "", "", "", "single crystal(200*350*10 um3)", "", "", "Fluctuation effects in the organic superconductor k-(BEDT-TTF)2Cu(NCS)2", "1996", "", "Laboratoire de Physique des Solides, URA 2 CNRS,Universite' Paris-Sud, F-91405 Orsay-Cedex, France", "Physica C,259(1996)181-186", "C. Pasquier,C.Pasquier,D. je'rome,D.Jerome,S. Friemel,S.Friemel,Y. Loirat,Y.Loirat", "", "" ] }, { "id": "30", "line_start": 32, "line_end": 32, "sha256": "0eafc42f7288ca325a37c7e0398f8bc70b3236fff58af7997621c90b8a2f76e6", "values": [ "30", "PHC2590181", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.4", "", "", "0", "", "", "", "", "", "", "", "", "57", "0.7", "122", "", "", "", "", "", "", "", "", "", "", "", "single crystal(125*400*20 um3)", "", "", "Fluctuation effects in the organic superconductor k-(BEDT-TTF)2Cu(NCS)2", "1996", "", "Laboratoire de Physique des Solides, URA 2 CNRS,Universite' Paris-Sud, F-91405 Orsay-Cedex, France", "Physica C,259(1996)181-186", "C. Pasquier,C.Pasquier,D. je'rome,D.Jerome,S. Friemel,S.Friemel,Y. Loirat,Y.Loirat", "", "" ] }, { "id": "31", "line_start": 33, "line_end": 33, "sha256": "b154fd0f6ae27696faf6aabe3af789d8d89f5b96092896683e9bafcd9259e9d4", "values": [ "31", "PRL0862130", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "magnetic phase diagram", "", "", "Quantum Melting of the Quasi-Two-Dimensional Vortex Lattice in kappa-(ET)2Cu(NCS)2", "2001", "", "", "Phys.Rev.Lett., 86(2001)2130", "J. S. Qualls,J.S.Brooks,M.M.Mola,S.Hill", "", "" ] }, { "id": "32", "line_start": 34, "line_end": 34, "sha256": "080bce4e251adfb43938a45f975b700c78a31fd694864e6699104931f4964fd7", "values": [ "32", "P063052506", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "5.2", "", "", "0", "", "", "", "", "", "", "", "", "", "1", "", "", "", "", "", "", "", "", "", "", "", "", "anisotropy factor = 800. penet(c) = 800 micron-m", "", "", "Unusual temperature dependence of the London penetration depth in all-organic beta-(ET)2SF5CH2CF2SO3 single crystals", "2001", "", "", "Phys.Rev.B, 63(2001)52506", "A.M.Kini,G.L.Gard,J.Mohtasham,J.Schlueter,R.Prozorov,R.W.Giannetta,R.W.Winter", "", "" ] }, { "id": "33", "line_start": 35, "line_end": 35, "sha256": "138e00eab4a0d218e86bfce6f67326d1b003c67a88445aa99f0f9f361d6a2fa6", "values": [ "33", "PHC3510261", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.34", "", "", "0", "3", "", "D", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (d8: substitution of all eight H atoms with D). delta-Tc = +0.27 +- 0.06 K.", "", "", "Universal inverse deuterium isotope effect on the Tc of BEDT-TTF-based molecular superconductors", "2001", "", "", "Physica C, 351(2001)261", "A.M.Kini,B.H.Ward,G.L.Gard,H.H.Wang,J.A.Schlueter,J.Mohtasham,R.W.Winter,U.Geiser", "", "" ] }, { "id": "34", "line_start": 36, "line_end": 36, "sha256": "1a54453edea1b1082625c3e8e34fa23c32f3fe082391258a8f666f7eb1791fb5", "values": [ "34", "PHB1430357", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.15", "", "", "0", "3", "0.28", "D", "", "", "", "2.48", "", "587", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (d8: substitution of all eight H atoms with D). delta-Tc = +0.28 K. Hc2(0)//b = 2.09, //c = 0.0806 T.", "", "", "", "1986", "", "", "Physica B, 143(1986)357", "C.-P.Heidmann,D.Schweitzer,K.Andres", "", "" ] }, { "id": "35", "line_start": 37, "line_end": 37, "sha256": "f2e4feb2fd76f3167084da066f8774dfb956d2800cbd793b38666e0913ff9220", "values": [ "35", "PHB1430334", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "7", "", "", "0", "2", "", "D", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC35", "", "", "", "", "isotope (d8: substitution of all eight H atoms with D). delta-Tc = (-) K.", "", "", "", "1986", "", "", "Physica B, 143(1986)334", "H.Schwenk,H.Veith,K.Andres", "", "" ] }, { "id": "36", "line_start": 38, "line_end": 38, "sha256": "ccf13788238258920937211f95e0188b87963b7566f96d20a0c317430d12c807", "values": [ "36", "ACP3140563", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "1", "", "C", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (substitution of the central double bonded C atoms with C<13>). delta-Tc = -0.6 K.", "", "", "", "1992", "", "", "C.R.Acad.Sci.Paris, 314(1992)563", "C.Bourbonnais,C.Lenoir,D.Jerome,J.-P.Buisson,P.Auban-Senzier,S.Lefrant,V.Merzhanov", "", "" ] }, { "id": "37", "line_start": 39, "line_end": 39, "sha256": "5433f9e7f7a6d000685165bcf15b677fce8e2f4054eef212f179b8d5eee6b578", "values": [ "37", "SYN0552542", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "3", "", "C", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (substitution of the central double bonded C atoms with C<13>). delta-Tc = -0.2 K.", "", "", "Isotope effect in superconductivity on <13>C substituted beta-(BEDT-TTF)2I3 ", "1993", "", "", "Synth.Met., 55-57(1993)2542", "C.Bourbonnais,C.Lenoir,D.Jerome,E.Canadell,P.Auban-Senzier,P.Batail", "", "" ] }, { "id": "38", "line_start": 40, "line_end": 40, "sha256": "097b1024cf8296d4e2ba12e133a4772c03b6cef516eb846db62a754418e9a753", "values": [ "38", "MCL2340127", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "6.95", "", "", "0", "2", "", "C", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (substitution of the central double bonded C atoms with C<13>). delta-Tc = 0 +- 0.1 K.", "", "", "The central bond <13>C=<13>C isotope effect for superconductivity in the high-Tc beta*-(ET)2I3 phase and its implications regarding the superconducting pairing mechanism in TTF-based organic superconductors", "1993", "", "", "Mol.Cryst.Liq.Cryst., 234(1993)127", "A.M.Kini,D.H.Parker,E.L.Venturini,H.H.Wang,J.A.Schlueter,J.D.B.Sutin,J.E.Schirber,J.M.Williams,J.R.Ferraro,K.D.Karlson,K.R.Lykke,P.Stout,P.Wurz,R.A.Klemm,S.K.Kumar,U.Geiser", "", "" ] }, { "id": "39", "line_start": 41, "line_end": 41, "sha256": "cb286046d2126ceac7c8e24c75d95f220e5db34b6db53136a54c450dfc5f1c16", "values": [ "39", "PHC2270010", 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substitution of all eight H atoms with D). delta-Tc = +1.0 K.", "", "", "Critical temperature (Tc) and crystal structures of kappa-(BEDT-TTF)2Ag(CN)2H2O (Tc=5K) and kappa-(BEDT-TTF-d8)2Ag(CN)2H2O (Tc=6K) ", "1993", "", "", "Synth.Met., 55-57(1993)2437", "H.Inokuchi,H.Mori,I.Hirabayashi,S.Tanaka,T.Mori,Y.Maruyama", "", "" ] }, { "id": "41", "line_start": 43, "line_end": 43, "sha256": "07f470a21721bbf3bc92114aa605bd01d79830429bc7bcd468cf78bf223533ee", "values": [ "41", "JPS0601426", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11.2", "", "", "0", "2", "", "D", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (d8: substitution of all eight H atoms with D). delta-Tc = -0.9 K.", "", "", "Isotope Effect in the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br ", "1991", "", "", "J.Phys.Soc.jpn, 60(1991)1426", "H.Anzai,M.Tokumoto,N.Kinoshita,Y.Tanaka", "", "" ] }, { "id": "42", "line_start": 44, "line_end": 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Substitution", "1991", "", "", "J.Phys.Soc.jpn, 60(1991)3230", "G.Saito,H.Ito,M.Watanabe,N.Hosoito,T.Ishiguro,T.Komatsu,Y.Nogami", "", "" ] }, { "id": "49", "line_start": 51, "line_end": 51, "sha256": "a77dfa34a31f7e3c3953282ff7222a6ed4bd82c02452d187f0c5a2c4b705368c", "values": [ "49", "SYN0270473", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "10.3", "", "", "0", "1", "", "D", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotope (d8: substitution of all eight H atoms with D). delta-Tc = +0.7 K.", "", "", "", "1988", "", "", "Synth.Met., 27(1988)A473", "G.Saito,H.Urayama,H.Yamochi,K.Oshima", "", "" ] }, { "id": "50", "line_start": 52, "line_end": 52, "sha256": "0749e9ddbcf1fba896d550dc089e5c816b052499ac6dd734819b6113fbe62a74", "values": [ "50", "MCL2290129", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "8.8", "", "", "0", "3", "", "D", "", "", "", "", "", "", "", "", "", "", "", 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Cass Avenue, Argonne, IL 60439, USA", "Physica.C,264(1996)81-94", "A.M. Kini,H.H. Wang,J.A. Schlueter,J.D. Dudek,Jack M. Williams,K.D. Carlson,K.R. Lykke,S.A. Sirchio,U. 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Kini,D. Nauman,J.A. Schlueter,J.D. Dudek,J.M. Williams,J.P. Flynn,M.E. Kelly,T. Roy,U. Geiser", "organic", "" ] }, { "id": "61", "line_start": 63, "line_end": 63, "sha256": "5ad5c7ea129caa02c29b91ab070139f078ac2145dddd354ea9eeb41183ece5cd", "values": [ "61", "PR02701947", "FSO3", "(TMTSF)2FSO3", "2", "TMTSF", "", "", "", "", "", "", "2.1", "2.1", "0.65", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermopower also measured.", "", "", "Metal-insulator transitions and superconductivity in ditetramethyltetraselenafulvalenium fluorosulfonate [(TMTSF)2FSO3]", "1983", "", "University of California,Los Angeles,USA", "Phys.Rev.B, 27(1983)1947", "E.Aharon-Shalom,F.Wudl,P.M.Chaikin,R.C.Lacoe,S.A.Wolf", "", "" ] }, { "id": "62", "line_start": 64, "line_end": 64, "sha256": "b0eee78a5960aed2929758a181f461d58a00ed51c5f4eb8962c34156976aeabf", "values": [ "62", "PR02900500", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "3.64", "", "", "", "", "", "", "", "", "", "", "gap from R measurement. R(max) at 24.5 K. R(min) at 7.72 K. Properties depend on anion ordering.", "", "", "Resistivity of the organic superconductor ditetramethyltetraselenafulvalenium perchlorate, (TMTSF)2ClO4, in its relaxed, quenched, and intermediate state", "1984", "", "", "Phys.Rev.B, 29(1984)500", "F.Wudl,H.Schwenk,K.Andres", "", "" ] }, { "id": "63", "line_start": 65, "line_end": 65, "sha256": "f7fb058a20c1e6f288c296e15f4b76f720919e3422c8883ca4e8442ce0077aef", "values": [ "63", "PR03103138", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.03", "", "", "0", "", "", "", "", "", "0.0358", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Hc1shows Hc1(0.115 K) = 0.358 Oe for H//ab-plane. For H//a, H//b, Hc1(0.115 K) are 0.052 and 0.087 Oe.", "", "", "New, organic, volume superconductor at ambient pressure", "1985", "", "", "Phys.Rev.B, 31(1985)3138", "C.P.Heidmann,D.Schweitzer,E.Hess,F.Gross,H.J.Keller,H.Schwenk,K.Andres", "", "" ] }, { "id": "64", "line_start": 66, "line_end": 66, "sha256": "01e60c81b3a654e4ede36a4ce3e7c49df492a746654dea7b05f922aa009ef61f", "values": [ "64", "PR03301987", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.5", "", "", "0", "", "", "", "-10", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC64", "", "", "", "", "hydrostatic pressure. anion length = 10.1 A", "OTC64.dat", "", "Shear-induced superconductivity in beta-di[bis(ethylenedithio)tetrathiafulvalene]triiodide [beta-(BEDT-TTF)2I3]", "1986", "", "", "Phys.Rev.B,33(1986)1987", "E.L.Venturini,H.H.Wang,J.E.Schirber,J.F.Kwak,J.M.Williams,L.J.Azevedo,M.A.Beno,P.C.W.Leung", "", "" ] }, { "id": "65", "line_start": 67, "line_end": 67, "sha256": "a980613600c39c71ad2e6d1eb5518f7713d48bc6f5630567830fcd9520b52c18", "values": [ "65", "PR03301987", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "", "", "", "", "", "", "2.8", "", "", "0", "", "", "", "-7.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC64", "", "", "", "", "hydrostatic pressure. anion length = 9.41 A", "OTC64.dat", "", "Shear-induced superconductivity in beta-di[bis(ethylenedithio)tetrathiafulvalene]triiodide [beta-(BEDT-TTF)2I3]", "1986", "", "", "Phys.Rev.B,33(1986)1987", "E.L.Venturini,H.H.Wang,J.E.Schirber,J.F.Kwak,J.M.Williams,L.J.Azevedo,M.A.Beno,P.C.W.Leung", "", "" ] }, { "id": "66", "line_start": 68, "line_end": 68, "sha256": "e313771cb1ad9fa1f097d21b05b091408a82efb7f95827065ce4341d40ea3479", "values": [ "66", "PR03301987", "AuI2", "beta-(BEDT-TTF)2AuI2", "2", "BEDT-TTF", "", "", "", "", "", "", "5", "", "", "0", "", "", "", "-12.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC64", "", "", "", "", "hydrostatic pressure. anion length = 9.36 A", "OTC64.dat", "", "Shear-induced superconductivity in beta-di[bis(ethylenedithio)tetrathiafulvalene]triiodide [beta-(BEDT-TTF)2I3]", "1986", "", "", "Phys.Rev.B,33(1986)1987", "E.L.Venturini,H.H.Wang,J.E.Schirber,J.F.Kwak,J.M.Williams,L.J.Azevedo,M.A.Beno,P.C.W.Leung", "", "" ] }, { "id": "67", "line_start": 69, "line_end": 69, "sha256": "4bc440fc5bef6375b999b77e3a1af5aa73021fa19c42f0c5ad9ea0121d6a3ff6", "values": [ "67", "PR03301987", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "0", "", "", "", "-7.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC67", "", "", "", "not hydrostatic pressure (using frozen cyclopentane). Tc(P=0) extraporated to 8 K. anion length = 10.1 A.", "", "OTC67.dat", "Shear-induced superconductivity in beta-di[bis(ethylenedithio)tetrathiafulvalene]triiodide [beta-(BEDT-TTF)2I3]", "1986", "", "", "Phys.Rev.B,33(1986)1987", "E.L.Venturini,H.H.Wang,J.E.Schirber,J.F.Kwak,J.M.Williams,L.J.Azevedo,M.A.Beno,P.C.W.Leung", "", "" ] }, { "id": "68", "line_start": 70, "line_end": 70, "sha256": "8c4a4577af67a105883ed300098845d2d6424c6e1298faf9ce3f75fb81bcd499", "values": [ "68", "L092067001", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1.45", "", "", "0", "", "", "", "", "", "", "5", "", "", "", "", "", "", "", "", "", "", "OHC68", "", "", "", "", "single crystal(triclinic). RRR=1400. H//b' (projection of b to ab-plane).", "OHC68.dat", "", "Magnetic determination of Hc2 under accurate alignment in (TMTSF)2ClO4", "2004", "", "", "Phys.Rev.Lett., 92(2004)67001", "J.I.Oh,M.J.Naughton", "", "" ] }, { "id": "69", "line_start": 71, "line_end": 71, "sha256": "00d6e21a0f6cbf36ed7c2c64d4e32e2d5a2b8fd06bb3143b6b5fd67ba2766a8b", "values": [ "69", "PR03403156", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "", "", "", "", "", "", "2.42", "", "", "0", "", "", "", "", "", "0.39", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Hc1,GL-par in TBL are ones at T=0.5K. Hc1(0.5K)//c = 16.5 Oe(1.65 mT).", "", "", "Superconductivity in sulfur-based organic superconductors: A volume property", "1986", "", "", "Phys.Rev.B, 34(1986)3156", "H.Schwenk,R.L.Greene,S.S.P.Parkin,V.Y.Lee", "", "" ] }, { "id": "70", "line_start": 72, "line_end": 72, "sha256": "f3317b83d0d6ea4523bb5b84495d1418d16164ecca5d9d13b485109c744c7792", "values": [ "70", "PR03403156", "AuI2", "beta-(BEDT-TTF)2AuI2", "2", "BEDT-TTF", "", "", "", "", "", "", "4.02", "", "", "0", "", "", "", "", "", "4", "6.63", "", "249", "0.51", "10.5", "", "", "", "", "", "", "OHC70", "", "", "", "", "Hc1, GL-par in TBL are ones at T=1.2K. Hc1(1.2K)//c=20.5 Oe. Hc2(0)//c=0.51 T. cohere//c=19.2 A. penet//c=4.1 um.", "OHC70.dat", "", "Superconductivity in sulfur-based organic superconductors: A volume property", "1986", "", "", "Phys.Rev.B, 34(1986)3156", "H.Schwenk,R.L.Greene,S.S.P.Parkin,V.Y.Lee", "", "" ] }, { "id": "71", "line_start": 73, "line_end": 73, "sha256": "4448794308992635eb737fce15cb4e92cb681eb378b6c37308bea0b1b05247fa", "values": [ "71", "PRL0500270", "ReO4", "beta-(BEDT-TTF)4(ReO4)2", "2", "BEDT-TTF", "7.78", "12.59", "16.97", "73.01", "79.89", "89.06", "1.9", "1.9", "0.4", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH71", "", "", "", "", "", "OPH71.dat", "", "Superconductivity in a new family of organic conductors", "1983", "", "", "Phys.Rev.Lett., 50(1983)270", "E.M.Engler,J.C.Scott,R.L.Greene,R.Lagier,R.R.Schumaker,S.S.P.Parkin,V.Y.Lee", "", "" ] }, { "id": "72", "line_start": 74, "line_end": 74, "sha256": "ad56c598f81fef3947a1e37d95d73bcedd338ba5d0b1a01709703ed052463d0d", "values": [ "72", "JPS0540869", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "6.609", "9.083", "15.267", "85.63", "95.62", "70.22", "1.1", "", "", "0", "", "", "", "", "", "", "1.78", "", "633", "", "", "", "", "", "", "", "", "OHC72", "", "", "", "", "Hc2(0.5K)//a=0.97T, Hc2(0.5K)//b'=0.93T, Hc2(0.5K)//c*=840Oe, where c* and b' are perpendicular to ab- and ac*-plane. cohere//b = 608A, cohere//c* = 29A.", "OHC72.dat", "", "Critical field anisotropy in an organic superconductor beta-(BEDT-TTF)2I3", "1985", "", "", "J.Phys.Soc.Jpn, 54(1985)869", "G.Saito,H.Anzai,H.Bando,K.Kajimura,K.Murata,M.Tokumoto,T.Ishiguro", "", "" ] }, { "id": "73", "line_start": 75, "line_end": 75, "sha256": "16cf0d9084639c846fab3c306853a057ac8e2bb75c7c59d17f60771d0e94e4fa", "values": [ "73", "JPS0541669", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "6.593", "8.975", "15.093", "93.79", "94.97", "110.54", "2.3", "", "", "0", "", "", "", "", "", "", "3.22", "1.4", "463", "", "", "", "", "", "", "", "", "OHC73", "", "", "", "", "Hc2(1.5K)//a=1.12T, Hc2(1.5K)//c*=450Oe, cohere//b'=444A, cohere//c*=18.5A, where c* and b' are perpendicular to ab- and ac*-plane.", "OHC73.dat", "", "Critical field anisotropy in an organic superconductor beta-(BEDT-TTF)2IBr2", "1985", "", "", "J.Phys.Soc.Jpn, 54(1985)1669", "G.Saito,H.Anzai,H.Bando,K.Kajimura,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "74", "line_start": 76, "line_end": 76, "sha256": "8f12d3b176d3f4fc6ca2a9db3706665b84993f19c8708568224d9639b8a207ea", "values": [ "74", "JPS0541669", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "6.593", "8.975", "15.093", "93.79", "94.97", "110.54", "2.2", "", "", "0", "", "", "", "", "", "", "", "", "515", "", "", "", "", "", "", "", "", "OHC74", "", "", "", "", "Hc2(0)//b'=3.77T from dHc2//b'/dT = 1.71T/K. Hc2(1.5K)//b'=1.20T, Hc2(1.5K)//c*=500Oe, cohere//b'=494A, cohere//c*=20.7A, where c* and b' are perpendicular to ab- and ac*-plane.", "OHC74.dat", "", "Critical field anisotropy in an organic superconductor beta-(BEDT-TTF)2IBr2", "1985", "", "", "J.Phys.Soc.Jpn, 54(1985)1669", "G.Saito,H.Anzai,H.Bando,K.Kajimura,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "75", "line_start": 77, "line_end": 77, "sha256": "ef3b763209c220310507d1018392dbb09b42f1788a4ecf55a3d74c786306abf8", "values": [ "75", "JPS0542084", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "", "", "", "", "", "", "", "", "125", "", "", "", "", "", "", "", "", "", "", "", "", "", "stable s/c at P=0 when P is released after P > 1.3 kbar measurements. Low Tc(1.5K)- and high Tc(8K)- phases observed.", "", "", "Pressure phase diagram of the organic superconductor beta-(BEDT-TTF)2I3", "1985", "", "", "J.Phys.Soc.Jpn, 54(1985)2084", "G.Saito,H.Anzai,H.Bando,K.Kajimura,K.Murata,M.Tokumoto,T.Ishiguro", "", "" ] }, { "id": "76", "line_start": 78, "line_end": 78, "sha256": "e76b32b88898026df68dba17047e3f791917de79981711927c624604799c648c", "values": [ "76", "JPS0570730", "Cu(NCS)2", "beta-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "16.248", "8.44", "13.124", "", "110.3", "", "10.4", "", "", "0", "", "", "", "", "", "", "", "", "9.6", "", "", "", "", "", "", "", "", "OHC76", "", "", "", "", "cohere< c > =182 A.", "OHC76.dat", "", "Peculiar critical field behaviour in the recently discovered ambient pressure organic superconductor (BEDT-TTF)2Cu(NCS)2 (Tc=10.4 K)", "1988", "", "", "J.Phys.Soc.Jpn, 57(1988)730", "G.Saito,H.Urayama,H.Yamochi,K.Oshima", "", "" ] }, { "id": "77", "line_start": 79, "line_end": 79, "sha256": "c8e13cfe94192d5225b03d338114803815731052bbc0b382afbb0baacb319cbe", "values": [ "77", "PHB1430366", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.1", "6", "0.13", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC77", "", "", "", "", "Hc2(T) at P=1.3 kbar.", "OHC77.dat", "", "Upper critical field of beta-(BEDT-TTF)2I3 in the high Tc superconducting state", "1986", "", "", "Physica B, 143(19686)366", "G.Saito,H.Anzai,K.Kajimura,K.Murata,M.Tokumoto,N.Toyota,S.Morita,T.Ishiguro,Y.Muto", "", "" ] }, { "id": "78", "line_start": 80, "line_end": 80, "sha256": "ec4dbd954b0b1073725e2872439a2331936a05b477ac211e5b553fd2471fdaa3", "values": [ "78", "SSC0570089", "AuI2", "beta-(BEDT-TTF)2AuI2", "2", "BEDT-TTF", "6.603", "9.015", "15.403", "94.95", "96.19", "110.66", "4.12", "", "", "0", "", "", "", "", "", "", "6.14", "", "177", "", "", "", "", "", "", "", "", "", "", "", "", "", "Hc2(0)//c = 1.1 T. cohere < c > = 30 A. Tc(max) = 4.98 K obtained for the same batch.", "", "", "Ambient pressure superconductivity at 4-5 K in beta-(BEDT-TTF)2AuI2", "1986", "", "", "Solid State Commun., 57(1986)89", "G.W.Crabtree,H.H.Wang,J.M.Williams,K.D.Carlson,K.S.Webb,L.Nunez,M.A.Beno,M.A.Firestone,U.Geiser", "", "" ] }, { "id": "79", "line_start": 81, "line_end": 81, "sha256": "f7ade6a66ab386b4264cdd7b924df1ae0092a7de1b73a3432c8b3aa50bedf139", "values": [ "79", "SSC0640335", "Cl2/2H2O", "(BEDT-TTF)3Cl2/2H2O", "2", "BEDT-TTF", "", "", "", "", "", "", "1.9", "1.9", "1.6", "1.5", "1", "", "", "", "", "", "", "0.21", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "dHc2/dT = 1.66 and 0.21 T/K for H//c and H//b*, respectively. Hc2(T) at 1.6 GPa.", "", "", "SUPERCONDUCTIVITY IN (BEDT-TTF)3CL22H2O", "1987", "", "", "SOLID STATE COMMUN.,64(1987)335", "H.Inokuchi,HIROO INOKUCHI,T.Mori,TAKEHIKO MORI", "", "" ] }, { "id": "80", "line_start": 82, "line_end": 82, "sha256": "25344a289123ee74abd98bdab9bde90207db6c857159e76520bd50b8e64dbd1b", "values": [ "80", "PHB1430378", "Ni(dmit)2", "TTF[Ni(dmit)2]2", "2", "TTF", "46.22", "3.732", "22.86", "", "119.29", "", "1.62", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "monoclinic. space-G = 2/c. RRR=90.", "", "", "The first 3d molecular superconductor under pressure ?: TTF[Ni(dmit)2]2", "1986", "", "", "Physica B, 143(19686)378", "L.Brossard,L.Valade,M.Ribault,P.Cassoux", "", "" ] }, { "id": "81", "line_start": 83, "line_end": 83, "sha256": "eab785acc5a6f93497e945723c6c81a42974454865f7ff1c4d5be6b1dbaa1770", "values": [ "81", "PHB1350515", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "2", "", "620", "", "", "", "", "", "", "", "", "", "", "", "", "", "Hc2(0)//c* = 0.08T. cohere=608A, cohere=29A.", "", "", "High Tc superconducting state in (BEDT-TTF)2 trihalides", "1985", "", "", "Physica B, 135(1985)515", "G.Saito,H.Anzai,H.Bando,H.Tanino,K.Kajimura,K.Murata,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "82", "line_start": 84, "line_end": 84, "sha256": "5739dfff9fe96a4b3a0f9709df70448a7237fb15720b67f9c1dc5da85034d1b0", "values": [ "82", "PHB1350515", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "7.2", "", "", "0", "", "", "", "", "", "", "25", "", "125", "", "", "", "", "", "", "", "", "", "", "", "", "", "s/c measured at P=1.6 GPa. Hc2(0)//C: = 2.7T. cohere=10A.", "", "", "High Tc superconducting state in (BEDT-TTF)2 trihalides", "1985", "", "", "Physica B, 135(1985)515", "G.Saito,H.Anzai,H.Bando,H.Tanino,K.Kajimura,K.Murata,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "83", "line_start": 85, "line_end": 85, "sha256": "c4ff8800bda0277f222f5d3f1c0eb7ae50d59cbd88a0743c1b1ac8e129f08464", "values": [ "83", "PHB1350515", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "", "", "", "", "", "", "2.3", "", "", "0", "", "", "", "", "", "", "", "", "460", "", "", "", "", "", "", "", "", "", "", "", "", "", "cohere=440A, cohere=19A at P=0 GPa. Tc(P=0.22GPa) = 0.8 K.", "", "", "High Tc superconducting state in (BEDT-TTF)2 trihalides", "1985", "", "", "Physica B, 135(1985)515", "G.Saito,H.Anzai,H.Bando,H.Tanino,K.Kajimura,K.Murata,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "84", "line_start": 86, "line_end": 86, "sha256": "b17cafb1e9f01b7df8322a4bad0872c6df589fb17d6d0e127198135e3cd157c1", "values": [ "84", "PHB1350515", "I2Br", "beta-(BEDT-TTF)2I2Br", "2", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not s/c. at P=0.3 GPa, down to 50 mK.", "", "", "High Tc superconducting state in (BEDT-TTF)2 trihalides", "1985", "", "", "Physica B, 135(1985)515", "G.Saito,H.Anzai,H.Bando,H.Tanino,K.Kajimura,K.Murata,M.Tokumoto,N.Kinoshita,T.Ishiguro", "", "" ] }, { "id": "85", "line_start": 87, "line_end": 87, "sha256": "7e3377d919ab6e30dd8de25c6c3f6a6306f62a0ca1ae039dcacfbbd8fb8e3fac", "values": [ "85", "PHB1430357", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.15", "", "", "0", "", "", "", "", "", "", "2.09", "", "587", "", "", "", "", "", "", "", "", "", "", "", "", "", "low-Tc-phase. Hc2//b = 2.48T, Hc2//c* = 0.081T. cohere< b > = 696A, cohere< c* > = 22.6A.", "", "", "", "1986", "", "", "Physica B, 143(1986)357", "C.-P.Heidmann,D.Schweitzer,K.Andres", "", "" ] }, { "id": "86", "line_start": 88, "line_end": 88, "sha256": "907bdbb0c86be6486cab5bd21912489ca804f023fe7b9fc986039bfb887c800f", "values": [ "86", "PHB1430357", "I3", "beta-(d-BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "1.43", "", "", "0", "", "", "", "", "", "", "2.58", "", "506", "", "", "", "", "", "", "", "", "", "", "", "", "", "low-Tc-phase. isotope (H to D exchange) sample. Hc2//b = 2.55T, Hc2//c* = 0.13T. cohere< b > = 500A, cohere< c* > = 25.5A.", "", "", "", "1986", "", "", "Physica B, 143(1986)357", "C.-P.Heidmann,D.Schweitzer,K.Andres", "", "" ] }, { "id": "87", "line_start": 89, "line_end": 89, "sha256": "478e9c8c779f2689a249a069bad6f4c0cef60ea648ac1413d7a7e921d87fd6e0", "values": [ "87", "SSC0660405", "AuBr2", "kappa-(DMET)2AuBr2", "2", "DMET", "11.542", "8.238", "16.168", "90", "90.99", "90", "1.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "rhombus-like crystal is s/c. others not s/c.", "", "", "Polymorphism and electrical conductivity of the organic superconductor (DMET)2AuBr2", "1988", "", "", "Solid State Commun., 66(1988)405", "H.Anzai,I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,Y.Honda,Y.Ishikawa", "", "" ] }, { "id": "88", "line_start": 90, "line_end": 90, "sha256": "177cfaf24e2492353ffa2d65d6542329e33c87c41d4c6b07bc199ab6f5c65f1f", "values": [ "88", "JPS0563436", 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56(1987)3436", "I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,T.Namiki,Y.Honda", "", "" ] }, { "id": "90", "line_start": 92, "line_end": 92, "sha256": "87a21ae21c8563bb71a22811c2cccf0e15e99bf0a728b3644d8eba798fdbd91d", "values": [ "90", "JPS0563436", "IBr2", "beta-(DMET)2IBr2", "2", "DMET", "", "", "", "", "", "", "0.58", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "On ambient-pressure superconductivity in organic conductors: Electrical properties of (DMET)2I3, (DMET)2I2Br and (DMET)2IBr2", "1987", "", "", "J.Phys.Soc.Jpn, 56(1987)3436", "I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,T.Namiki,Y.Honda", "", "" ] }, { "id": "91", "line_start": 93, "line_end": 93, "sha256": "3149636aff50c5c155fe2f960150dd8f7615a3460f731fb028b33211829b7b65", "values": [ "91", "PHB1430360", "AuI2", "beta-(BEDT-TTF)2AuI2", "2", "BEDT-TTF", "", "", "", "", "", "", "3.18", "", "", "", "", "", "", "-11", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Meissner effect under pressure in organic superconductors of the beta-(BEDT-TTF)2X family (X = I3, IBr2, AuI2)", "1986", "", "", "Physica B, 143(19686)360", "C.-P.Heidmann,E.Amberger,F.Gross,H.Fuchs,H.Veith,K.Andres", "", "" ] }, { "id": "92", "line_start": 94, "line_end": 94, "sha256": "00d0d30fd8d1da54e4aea62ea594fd1b13358c09c16c5987cecef25448200bed", "values": [ "92", "PHB1430360", "IBr2", "beta-(BEDT-TTF)2IBr2", "2", "BEDT-TTF", "", "", "", "", "", "", "1.95", "", "", "", "", "", "", "-13.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Meissner effect under pressure in organic superconductors of the beta-(BEDT-TTF)2X family (X = I3, IBr2, AuI2)", "1986", "", "", "Physica B, 143(19686)360", "C.-P.Heidmann,E.Amberger,F.Gross,H.Fuchs,H.Veith,K.Andres", "", "" ] }, { "id": "93", "line_start": 95, "line_end": 95, "sha256": "cd5c00b0e6f9283c3312ad0ac1e44175c69930aa8cf543e8b5bd188554f4ea4d", "values": [ "93", "PRL0491008", "ReO4", "(TMTSF)2ReO4", "", "TMTSF", "", "", "", "", "", "", "1.3", "1.3", "0.95", "0.95", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Order-disorder transition at 180K.", "", "", "X-Ray Scattering Evidence for Anion Ordering and Structural Distortions in the Low-Temperature Phase of Di(Tetramethyltetraselanafulvalenium) Perrhenate [(TMTSF)2ReO4]", "1982", "", "", "Phys.Rev.Lett., 49(1982)1008", "J.P.Pouget,K.Bechgaard,R.Comes,R.Moret", "", "" ] }, { "id": "94", "line_start": 96, "line_end": 96, "sha256": "3ecad076949c83932de843dd6e36b30f8d258b7a4f6e25476222f68b2889f6ae", "values": [ "94", "PHC4020017", "Cu(NCS)2", "kappa-(d8-(BEDT-TTF))2Cu(SCN)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.6", "", "", "0", "", "", "", "-38.8", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC94", "", "", "", "", "substitution of all eight H atoms with D. static pressure. not s/c down to 1.25 K at P=5.74 kbar.", "OTC94.dat", "", "Comparative pressure studies of the superconducting transition temperature in isotopically substituted samples of kappa-(BEDT-TTF)2Cu(SCN)2", "2004", "", "Department of Physics, Clarendon Laboratory, Oxford University, Parks Road, Oxford OX1 3PU, UK", "Physica C, 402(2004)17", "A.-K.Klehe,A.M.Kini,J.A.Schlueter,J.S.Schilling,T.Tomita", "", "" ] }, { "id": "95", "line_start": 97, "line_end": 97, "sha256": "482ed1e28917440a932d94d2244343c59f0a824c525d3441139f54f9497ba26b", "values": [ "95", "PHC4020017", "Cu(NCS)2", "kappa-(<2>H8<13>C4<34>S8-(BEDT-TTF))2Cu(SCN)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.4", "", "", "0", "", "", "", "-38.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC95", "", "", "", "", "multi-isotope D, C, S (substitution of all eight H atoms with D, substitution of the four ethylene C atoms with C<13>, substitution of all eight S atoms with S<34>). static pressure.", "OTC95.dat", "", "Comparative pressure studies of the superconducting transition temperature in isotopically substituted samples of kappa-(BEDT-TTF)2Cu(SCN)2", "2004", "", "Department of Physics, Clarendon Laboratory, Oxford University, Parks Road, Oxford OX1 3PU, UK", "Physica C, 402(2004)17", "A.-K.Klehe,A.M.Kini,J.A.Schlueter,J.S.Schilling,T.Tomita", "", "" ] }, { "id": "96", "line_start": 98, "line_end": 98, "sha256": "b2cec2e168d9e6e872640a9474cd123bd08130b285804c4615e77396815485b9", "values": [ "96", "PRL0451449", "PF6", "(TMTSF)2PF6", "2", "TMTSF", "", "", "", "", "", "", "1.3", "1.3", "0.65", "0.65", "", "", "", "-0.87", "0.02", "0.6", "0.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Semiconducting at P=0.48 GPa.. Hc1, Hc2 are for H//c, at P=1.77 GPa(Tc=0.6 K).", "", "", "Observation of the Meissner effect in an organic superconductor", "1980", "", "", "Phys.Rev.Lett., 45(1980)1449", "A.L.Stevens,D.B.McWhan,D.Nalewajek,F.Wudl,G.A.Thomas,K.Andres", "", "" ] }, { "id": "97", "line_start": 99, "line_end": 99, "sha256": "5c928829ea039973048b38c621208746b07746b761a32908e6ea20006f273bba", "values": [ "97", "PRL0451587", "PF6", "(TMTSF)2PF6", "2", "TMTSF", "", "", "", "", "", "", "1.1", "1.1", "0.65", "0.65", "", "", "", "-0.8", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at 6 K under P=0.65 GPa.", "", "", "Pressure dependence of superconductivity in an organic superconductor bis-tetramethyltetraselenafulvalence hexafluorophosphate", "1980", "", "", "Phys.Rev.Lett., 45(1980)1587", "E.M.Engler,R.L.Greene", "", "" ] }, { "id": "98", "line_start": 100, "line_end": 100, "sha256": "3f7a141221b5dff0990c277db31fb77e2f767c1c6eb12dd01e2e90e62951e56d", "values": [ "98", "PRL0491346", "ClO4", "(TMTSF)2ClO4", "", "TMTSF", "", "", "", "", "", "", "1.221", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "14", "213", "", "", "", "", "", "", "", "(delta-C/gamma*Tc) = 1.67.", "", "", "Influence of the cooling rate on the superconducting properties of the organic solid di-tetramethyltetraselenafulvalenium-perchlorate, (TMTSF)cClO4", "1982", "", "", "Phys.Rev.Lett., 49(1982)1346", "K.Bechgaard,P.Garoche,R.Brusetti", "", "" ] }, { "id": "99", "line_start": 101, "line_end": 101, "sha256": "e3d010f45462dfa72aaaa6bebbd7b2dafc8327cbea571b783775d46c053e6289", "values": [ "99", "MCL0790283", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1", "", "", "", "", "", "", "", "", "", "", "", "600", "", "", "", "", "", "", "", "", "", "", "", "", "", "cohere< b > = 540 A, cohere< c* > = 60 A calculated from dHc2/dT.", "", "", "Superconducting transition of (TMTSF)2ClO4 in magnetic fields", "1982", "", "", "Mol.Crys.Liq.Crys., 79(1982)283", "G.Saito,H.Anzai,K.Kajimura,K.Murata,T.Ishiguro", "", "" ] }, { "id": "100", "line_start": 102, "line_end": 102, "sha256": "f12dbb10a7212a06eba69dc1d10216b82884965e371f0c5d6b559209d5523d28", "values": [ "100", "MCL0790183", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Some properties of the (TMTSF)2X superconductors", "1982", "", "", "Mol.Crys.Liq.Crys., 79(1982)183", "E.M.Engler,M.Y.Choe,P.Haen,P.M.Chaikin,R.L.Greene,S.Z.Huang", "", "" ] }, { "id": "101", "line_start": 103, "line_end": 103, "sha256": "404e67d910157fb7d6d9a5ee80a7fcfb6a8000a2f31ea50b13dd2f88c419b911", "values": [ "101", "MCL0790183", "PF6", "(TMTSF)2PF6", "2", "TMTSF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Some properties of the (TMTSF)2X superconductors", "1982", "", "", "Mol.Crys.Liq.Crys., 79(1982)183", "E.M.Engler,M.Y.Choe,P.Haen,P.M.Chaikin,R.L.Greene,S.Z.Huang", "", "" ] }, { "id": "102", "line_start": 104, "line_end": 104, "sha256": "0ce69bc053863fa50be8f092b6b298a45cf533c4e3d4b9a31d2ab1f095cc1561", "values": [ "102", "MCL1190241", "ReO4", "(TMTSF)2ReO4", "2", "TMTSF", "", "", "", "", "", "", "1.52", "", "", "1.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "rapid cooling sample. M-I transition at 180 K. For slow cooling sample, Tc(P=10 kbar)=1.46 K.", "", "", "Influence of the anion order on the ground state of the organic conductor (TMTSF)2ReO4", "1985", "", "", "Mol.Cryst.Liq.Cryst., 119(1985)241", "", "", "" ] }, { "id": "103", "line_start": 105, "line_end": 105, "sha256": "3fe84be52c6f2637f7cd856cc77112b0db328d146e6c9e65b228be973c2eccd1", "values": [ "103", "JPL0410095", "PF6", "(TMTSF)2PF6", "2", "TMTSF", "", "", "", "", "", "", "0.9", "", "", "1.2", "", "", "", "", "", "", "0.014", "0.0222", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "H perpendicular to layer. G-L = 3 estimated. s/c determined by resistivity.", "", "", "Superconductivity in a synthetic organic conductor (TMTSF)2PF6", "1980", "", "", "J.Phys.Lett., 41(1980)L-95", "A.Mazaud,D.Jerome,K.Bechgaard,M.Ribault", "", "" ] }, { "id": "104", "line_start": 106, "line_end": 106, "sha256": "8817f335c0fb7fbf41ca329eaf8209cf3ddfa703ad9ab1c89a1aa4791238b74c", "values": [ "104", "PR0240478", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1", "", "", "0", "", "", "", "", "", "", "2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc defined as R/Rn=0.5. Hc2 is for H//chain axis. For H perpendicular to chain, Hc2(0)=1.5 kOe.", "", "", "Magnetic susceptibility and resistive transitions of superconducting (TMTSF)2ClO4: Critical magnetic fields", "1981", "", "", "Phys.Rev.B, 24(1981)478", "A.N.Bloch,D.O.Cowan,D.U.Gubser,L.-Y.Chiang,M.Lee,R.S.Potember,T.O.Poehler,W.W.Fuller", "", "" ] }, { "id": "105", "line_start": 107, "line_end": 107, "sha256": "2e6c17a0402b2afac6902f86d48a65314202d7194b467717f99bdd722ee70352", "values": [ "105", "MCL0790001", "PF6", "(TMTSF)2PF6", "", "TMTSF", "7.297", "7.711", "13.522", "83.39", "86.27", "71.01", "0.9", "", "", "0.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "anion symmetry = octa. M-I transition at 12-17 K.", "", "", "TMTSF2X salts. Preparation, structure, and effect of the anion", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)1", "K.Bechgard", "", "" ] }, { "id": "106", "line_start": 108, "line_end": 108, "sha256": "831462422fafd6a816552127f8412560901a6f8cb82293303fd16eebf078b421", "values": [ "106", "MCL0790001", "AsF6", "(TMTSF)2AsF6", "", "TMTSF", "", "", "", "", "", "", "1.1", "", "", "1.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "anion symmetry = octa. M-I transition at 12-16 K.", "", "", "TMTSF2X salts. Preparation, structure, and effect of the anion", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)1", "K.Bechgard", "", "" ] }, { "id": "107", "line_start": 109, "line_end": 109, "sha256": "74bd13511cf0c947bb75e6ff45db81c6f3e52370e5909b494c01fb2bcfb9b6f6", "values": [ "107", "MCL0790001", "SbF6", "(TMTSF)2SbF6", "", "TMTSF", "7.299", "7.728", "13.901", "82.77", "85.23", "71.52", "0.4", "", "", "1.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "anion symmetry = octa. M-I transition at 17 K.", "", "", "TMTSF2X salts. Preparation, structure, and effect of the anion", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)1", "K.Bechgard", "", "" ] }, { "id": "108", "line_start": 110, "line_end": 110, "sha256": "7c2be850287371fee6a35ac4974334c05566c5c2f75fb2cfbc13ab7cc8c827a4", "values": [ "108", "MCL0790001", "TaF6", "(TMTSF)2TaF6", "", "TMTSF", "7.28", "7.716", "13.918", "82.88", "85.37", "71.67", "1.4", "", "", "1.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "anion symmetry = octa.", "", "", "TMTSF2X salts. Preparation, structure, and effect of the anion", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)1", "K.Bechgard", "", "" ] }, { "id": "109", "line_start": 111, "line_end": 111, "sha256": "f4e66aab56c16703f9a1303c8f1df5f3751368665944e1acd6e8b77ae319fa7f", "values": [ "109", "MCL0790001", "NbF6", "(TMTSF)2NbF6", "", "TMTSF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at 12 K. not s/c upto 12 kbar(1.2 GPa).", "", "", "TMTSF2X salts. Preparation, structure, and effect of the anion", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)1", "K.Bechgard", "", "" ] }, { "id": "110", "line_start": 112, "line_end": 112, "sha256": "354657939ec2aca00c80d81af5796c43c27215b107ec48c0d242061adf3883c3", "values": [ "110", "JPL0410607", "AsF6", "(TMTSF)2AsF6", "2", "TMTSF", "", "", "", "", "", "", "1.1", "", "", "1.2", "", "", "", "", "", "", "", "0.055", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "H perpendicular to chain.", "", "", "Superconductivity and absence of a Kohn anomaly in the quasi-one-dimensional organic conductor: (TMTSF)2AsF6", "1980", "", "", "J.Phys.Lett., 41(1980)L-607", "D.Jerome,J.-P.Pouget,K.Bechgaard,M.Ribault", "", "" ] }, { "id": "111", "line_start": 113, "line_end": 113, "sha256": "37c80f5becfea9acd7a56a10dc58a72d5c036608682c1710098aa4d418693206", "values": [ "111", "JPS0731434", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11.61", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC111", "", "", "", "", "slow cooled sample. H-D substitution effect.", "OTC111.dat", "", "Substitution Effect by Deuterated Donors on Superconductivity in kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2004", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 73(2004)1434", "N.Kobayashi,N.Yoneyama,T.Sasaki", "", "" ] }, { "id": "112", "line_start": 114, "line_end": 114, "sha256": "119ddb5f662f68a7481f5192d139d1d1d254f7a8ccc2cf439e900005be7ce1f7", "values": [ "112", "JPS0731434", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "9.94", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC112", "", "", "", "", "quenched sample. H-D substitution effect.", "OTC112.dat", "", "Substitution Effect by Deuterated Donors on Superconductivity in kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2004", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 73(2004)1434", "N.Kobayashi,N.Yoneyama,T.Sasaki", "", "" ] }, { "id": "113", "line_start": 115, "line_end": 115, "sha256": "40cc9cd22283ec08b04bfb2194c63483c7acf15ba2b5891c8d01dbb6bf850baf", "values": [ "113", "P068104504", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "5.2", "", "", "0", "", "", "", "13.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC113", "", "", "", "", "Tc(P) measured.", "OTC113.dat", "", "Pressure-induced insulating state in an organic superconductor", "2003", "", "Institut fur Festkorperpkysik, Technische Universitat Dresden, D-01062 Dresden, Germany", "Phys.Rev.B, 68(2003)104504", "C.Pfleiderer,G.L.Gard,J.A.Schlueter,J.Hagel,J.Mohtasham,J.Wosnitza", "", "" ] }, { "id": "114", "line_start": 116, "line_end": 116, "sha256": "c7ec210add7f2925f149dab0b0fca0934917ce2ebef2e683a586d0f60793d447", "values": [ "114", "PHC4020017", "Cu(NCS)2", "kappa-(h8-(BEDT-TTF))2Cu(SCN)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.17", "", "", "0", "", "", "", "-40.8", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC114", "", "", "", "", "not s/c down to 1.25 K at P=4.13 kbar.", "OTC114.dat", "", "Comparative pressure studies of the superconducting transition temperature in isotopically substituted samples of kappa-(BEDT-TTF)2Cu(SCN)2", "2004", "", "Department of Physics, Clarendon Laboratory, Oxford University, Parks Road, Oxford OX1 3PU, UK", "Physica C, 402(2004)17", "A.-K.Klehe,A.M.Kini,J.A.Schlueter,J.S.Schilling,T.Tomita", "", "" ] }, { "id": "115", "line_start": 117, "line_end": 117, "sha256": "aefce3ef954fe12895c964013a99525a15af16e8a9dec90825791ecb1d62be50", "values": [ "115", "SSC0711087", "Au(CN)2", "(DMET)2Au(CN)2", "2", "DMET", "", "", "", "", "", "", "1", "", "", "0.15", "", "", "", "-0.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SDW transition temp.(P=0) = 24.4 K. Structural transition at 180 K (P=0).", "", "", "Phase diagram of superconductivity and spin density wave in (DMET)2Au(CN)2", "1989", "", "", "Solid State Commu., 71(1989)1087", "I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,Y.Honda", "", "" ] }, { "id": "120", "line_start": 118, "line_end": 118, "sha256": "f802cb126bcdd4b40d3a97c59181cf813a3d3a5fc5f5d45c19db722c25fc4f98", "values": [ "120", "PR06111739", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.75", "", "", "0", "", "", "", "-16", "", "", "10.4", "", "144", "", "", "", "", "", "", "", "", "OTBL120", "OHC120", "", "", "", "hydrostatic pressure effect. Tc,Hc by thermal expansion measurements. Hc2(0) = 1.4 T for H//c. cohere = 7.9 A. anisotropy = 330", "OTBL120.dat", "OHC120.dat", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "121", "line_start": 119, "line_end": 119, "sha256": "3aff255d65ed49be8cea481dc5bca59cda4231311d0303bf91137e8ab4cfe3be", "values": [ "121", "PR06111739", "Cu(NCS)2", "kappa-(d8-BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "9.95", "", "", "0", "", "", "D", "-29", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTBL121", "", "", "", "", "details shown in Fig.", "OTBL121.dat", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "122", "line_start": 120, "line_end": 120, "sha256": "8bd09cbdf63eb1d4307bd518eac91bc931eb8df1a8b145b95ae437857b189fb0", "values": [ "122", "PR05703084", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.4", "", "", "0", "", "", "", "", "", "2", "3.4", "", "100", "", "59", "", "", "18.7", "221", "", "", "", "", "", "", "", "(delta-C/gamma*Tc) = 2.1. Sp-heat measured for H perpendicular to conduction layer.", "", "", "Specific heat and critical field of the organic superconductor %!\"-(BEDT-TTF)2SF5CH2CF2SO3", "1998", "", "Physikalisches Institut, Universitat Karlsruhe, D-76128 Karlsruhe, Germany", "Phys.RevB,57(1998)3084-3088", "D. Beckmann,D.Beckmann,G.L. Dard,G.L.Gard,J. Hagel,J. Wosniza,J.A. Schlueter,J.A.Schlueter,J.Hagel,J.M. Williams,J.M.Williams,J.Wosnitza,P.G. Nixon,P.G.Nixon,R.W. Winter,R.W.Winter,S. Wanka,S.Wanka", "", "" ] }, { "id": "123", "line_start": 121, "line_end": 121, "sha256": "156ca1143019650731e1d95e0178419efdf0b97a3fd27d352022b0d572025e98", "values": [ "123", "JPS0541236", "I3", "beta-(BEDT-TTF)2I3", "2", "BEDT-TTF", "", "", "", "", "", "", "8", "8", "0.13", "", "", "", "", "", "", "", "1.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isotropic. For H//c*, Hc2(T=1.5K,P=0.13GPa) = 1.3 T. Hc2(0)=1.7 T(linear extrapolation). P not given.", "", "", "Superconductivity with the onset at 8K in the organic conductor beta-(BEDT-TTF)2I3 under pressure", "1985", "", "", "J.Phys.Soc.Jpn, 54(1985)1236", "G.Saito,H.Anzai,H.Bando,K.Kajimura,K.Murata,M.Tokumoto,T.Ishiguro", "", "" ] }, { "id": "124", "line_start": 122, "line_end": 122, "sha256": "6ae6b25d72be8978f2cf010bc62e9ec497f93af7112c24ff42ea8e40170dec63", "values": [ "124", "JPS0720369", "GaCl4", "ramda-(BETS)2GaCl4", "", "BETS", "", "", "", "", "", "", "4.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Field-induced s/c. s/c for 17. SDW not observed.", "", "", "Superconductivity in (DMET)2AuCl2 and (DMET)2AuI2", "1987", "", "", "J.Phys.Soc.Jpn, 56(1987)4241", "H.Anzai,I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,T.Namiki,Y.Honda", "", "" ] }, { "id": "130", "line_start": 128, "line_end": 128, "sha256": "24ed934334cb8b8b9184a454a168bddded650396c32a72ca96e292f0d74231e3", "values": [ "130", "JPS0564241", "AuI2", "beta-(DMET)2AuI2", "2", "DMET", "", "", "", "", "", "", "0.55", "", "", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "R=R0*T**<1.32>. M-I transition at 20K (P=0).", "", "", "Superconductivity in (DMET)2AuCl2 and (DMET)2AuI2", "1987", "", "", "J.Phys.Soc.Jpn, 56(1987)4241", "H.Anzai,I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,T.Namiki,Y.Honda", "", "" ] }, { "id": "131", "line_start": 129, "line_end": 129, "sha256": "c03012e9cf5128cafa782ea5ba148a31b6ee0d84a04cae2ffc333c88af5ba0c4", "values": [ "131", "JPS0562627", "AuBr2", "beta-(DMET)2AuBr2", "2", "DMET", "", "", "", "", "", "", "1", "", "", "0.15", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(on) = 1.6 K under P=0.15 GPa. metal-semicond transition at 180 K (P=0).", "", "", "Superconductivity and the possibility of semiconductor-metal transition in (DMET)2AuBr2", "1987", "", "", "J.Phys.Soc.Jpn, 56(1987)2627", "I.Ikemoto,K.Kikuchi,K.Kobayashi,K.Murata,K.Saito,T.Ishiguro,T.Namiki,Y.Honda", "", "" ] }, { "id": "132", "line_start": 130, "line_end": 130, "sha256": "6eb26b72406025c5ada3cd50c056a33302007b5d1435073e9b51a4add34326e9", "values": [ "132", "PR0301282", "FSO3", "(TMTSF)2FSO3", "2", "TMTSF", "", "", "", "", "", "", "1.3", "1.6", "0.7", "0.5", "", "", "", "-1.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "anisotropic behaviour. Tc by susceptibility.", "", "", "Evidence for diamagnetism in (TMTSF)2FSO3 (bis-tetramethyltetrathiafulvalenium fluorosulfate) at low temperature under pressure", "1984", "", "", "Phys.Rev.B, 30(1984)1282", "F.Gross,F.Wudl,H.Schwenk,J.Brennan,K.Andres,S.D.Cox", "", "" ] }, { "id": "133", "line_start": 131, "line_end": 131, "sha256": "00257332a4d3b2cdb752db1e7d984f3be97e2cad8a1e1b7f3bde94f5d32db72f", "values": [ "133", "MCL0790155", "AsF6", "(TMTSF)2AsF6", "", "TMTSF", "", "", "", "", "", "", "1.1", "", "", "1.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition temp. = 12K (P=0).", "", "", "Organic superconductors: A survey of low dimensional phenomena", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)155", "D.Jerome", "", "" ] }, { "id": "134", "line_start": 132, "line_end": 132, "sha256": "f019407b899a28e359b0267a2b80c4c2641404903e147c0e64fcb2b928dc7d69", "values": [ "134", "MCL0790155", "PF6", "(TMTSF)2PF6", "", "TMTSF", "", "", "", "", "", "", "1.2", "", "", "0.85", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Organic superconductors: A survey of low dimensional phenomena", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)155", "D.Jerome", "", "" ] }, { "id": "135", "line_start": 133, "line_end": 133, "sha256": "29ffa10faacbbc1dddb3050972aa1153eac6ef41efa57a78d9489b471b23d314", "values": [ "135", "MCL0790155", "NO3", "(TMTSF)2NO3", "", "TMTSF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not s/c (P= 8 kbar, Tc < 50 mK). M-I transition temp = 11 K (P=0) go to 0 K at P=8 kbar.", "", "", "Organic superconductors: A survey of low dimensional phenomena", "1982", "", "", "Mol.Cryst.Liq.Cryst., 79(1982)155", "D.Jerome", "", "" ] }, { "id": "136", "line_start": 134, "line_end": 134, "sha256": "b5b5ba31f843d7ddf3b0ca5875e3192f7495999acc904d64bbbb988c7b279b28", "values": [ "136", "SSC1040571", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.46", "", "", "0", "", "", "", "-13.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc = 4.45 - 1.34*P + 0.056*P^2 (P in kbar).", "", "", "Dependence of Tc on hydrostatic pressure in beta''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2", "1997", "", "", "Solid State Commun., 104(1997)571", "G.L.Gard,G.Looney,J.A.Schlueter,J.M.Williams,J.S.Schilling,P.G.Nixon,R.W.Winter,S.Sadewasser", "", "" ] }, { "id": "137", "line_start": 135, "line_end": 135, "sha256": "3817fd80ae0b9847c021aae59e5861fcb7984bb6d83c15a9cd5463332791778a", "values": [ "137", "SYN0552865", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11", "", "", "0", "", "", "", "", "", "", "", "", "", "210", "", "", "", "", "", "", "", "", "", "", "", "", "penet// plane in micron-m.", "", "", "Magnetic penetration depth of the kappa-phase family of organic superconductors ", "1993", "", "", "Synth.Met., 55-57(1993)2865", "K.Ikeda,K.Kanoda,T.Takahashi,Y.Tsubokura,et al", "", "" ] }, { "id": "138", "line_start": 136, "line_end": 136, "sha256": "38c239aa81514718b8c13ede4a3c18448611ee84f5eb8a683e37c576f03e941a", "values": [ "138", "SYN0552865", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "2", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "210", "", "", "", "", "", "", "", "", "", "", "", "", "PENET// plane in micron-m.", "", "", "Magnetic penetration depth of the kappa-phase family of organic superconductors ", "1993", "", "", "Synth.Met., 55-57(1993)2865", "K.Ikeda,K.Kanoda,T.Takahashi,Y.Tsubokura,et al", "", "" ] }, { "id": "139", "line_start": 137, "line_end": 137, "sha256": "64f2b1e493b934731030aed87ccdf4d0726379f0dc21fa2e8ee3c20441effbda", "values": [ "139", "SYN0552865", "Ag(CN)2H2O", "kappa-(BEDT-TTF)2Ag(CN)2H2O", "2", "BEDT-TTF", "", "", "", "", "", "", "5", "", "", "0", "", "", "", "", "", "", "", "", "", "80", "", "", "", "", "", "", "", "", "", "", "", "", "PENET// plane in micron-m.", "", "", "Magnetic penetration depth of the kappa-phase family of organic superconductors ", "1993", "", "", "Synth.Met., 55-57(1993)2865", "K.Ikeda,K.Kanoda,T.Takahashi,Y.Tsubokura,et al", "", "" ] }, { "id": "140", "line_start": 138, "line_end": 138, "sha256": "c211dc89f9d53c4b238a40fef1958fcc1d93175666adf61b8f18acd1fac1d0e6", "values": [ "140", "SYN0552865", "AuI2", "kappa-(MDT-TTF)2AuI2", "2", "MDT-TTF", "10.797", "7.789", "28.991", "", "", "", "3.5", "", "", "0", "", "", "", "", "", "", "", "", "", "20", "", "", "", "", "", "", "", "", "", "", "", "", "PENET// plane in micron-m. Tc, structure data from Synth.Met., 27B(1988)379.", "", "", "Magnetic penetration depth of the kappa-phase family of organic superconductors ", "1993", "", "", "Synth.Met., 55-57(1993)2865", "K.Ikeda,K.Kanoda,T.Takahashi,Y.Tsubokura,et al", "", "" ] }, { "id": "141", "line_start": 139, "line_end": 139, "sha256": "755c5447bf8b55ca360b067682949f14aa53a32f9f03ac7cadb9e1580ed2c16a", "values": [ "141", "JPL0420051", "PF6", "(TMTSF)2PF6", "", "TMTSF", "", "", "", "", "", "", "0.9", "0.9", "0.9", "0.9", "", "", "", "-0.59", "", "", "", "0.008", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(P=24kbar) = 0.19K. TBL value of (dHc2/dT) is for P=24 kbar, H perpendicular. (dTc/dT) = 0.0222 T/K at P=12 kbar.", "", "", "Pressure dependence of the organic superconductivity in (TMTSF)2PF6", "1981", "", "", "J.Phys.Lett., 42(1981)L-51", "A.Mazaud,D.Jerome,H.J.Schulz,M.Ribault", "", "" ] }, { "id": "150", "line_start": 140, "line_end": 140, "sha256": "0fc63318f33b7478d01b1d85f31d44ea8c23d32f85b88659359a817c416fcc5d", "values": [ "150", "ACS1230306", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "11.787", "36.607", "8.504", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-5.5", "2.5", "OTC150", "", "", "", "", "structural transformation at 60-140 K. Coexistence of SC and AF. density = 2.751 g/cm3. Curie-C = 4.70 K.emu/mol.", "OTC150.dat", "", "A novel antiferromagnetic organic superconductor kappa-(BETS)2FeBr4 ", "2001", "", "", "J.Am.Chem.Soc., 123(2001)306", "A.Kobayashi,B.Zh.Narymbetov,E.Fujiwara,H.Fujiwara,H.Kobayashi,K.Kato,M.Tokumoto,P.Cassoux,Y.Nakazawa", "", "" ] }, { "id": "151", "line_start": 141, "line_end": 141, "sha256": "305a6db1ca3b17d961ad1752eadb6f248bcf8269fdaec0b8c71bf331bd50db71", "values": [ "151", "AC11712209", "[(H2O)Fe(C2O4)3]:PhCN", "beta''-(BEDT-TTF)2[(H2O)Fe(C2O4)3]:PhCN", "", "BEDT-TTF", "", "", "", "", "", "", "7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "PhCN=C6H5CN", "", "", "Superconducting and semiconducting magnetic charge transfer salts: (BEDT-TTF)4AFe(C2O4)3.C6H5CN (A=H2O, K, NH4)", "1995", "", "", "J.Am.Chem.Soc., 117(1995)12209", "A.W.Graham,F.L.Pratt,J.L.Caulfield,J.Singleton,L.Ducasse,M.B.Hursthouse,M.Kurmoo,P.Day,P.Guionneau,S.J.Coles,W.Hayes", "", "" ] }, { "id": "152", "line_start": 142, "line_end": 142, "sha256": "42ce2c2d01e449fb2eef6879bbf87dd7477e5db7a389f9b80e7ef575d7690da7", "values": [ "152", "P070094514", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1.4", "", "", "0", "", "", "", "", "", "", "16.3", "", "280", "", "", "", "", "", "", "", "", "OTC152-1", "OTC152-2", "", "", "", "Field-induced SC appear under high fields besides conventional SC. COHERE correspond to FISC. COHERE = 42 A.", "OTC152-1.dat", "OTC152-2.dat", "Magnetic-field-induced superconductivity in the antiferromagnetic organic superconductor kappa-(BETS)2FeBr4", "2004", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 70(2004)94514", "B.Zhang,H.Fujiwara,H.Kobayashi,K.Enomoto,M.Nishimura,S.Uji,S.Yasuzuka,T.Konoike,T.Terashima", "", "" ] }, { "id": "153", "line_start": 143, "line_end": 143, "sha256": "48035a4a587c487633d203ff06b88e70ceb7baa36450d5000d6f61d37f971150", "values": [ "153", "P070092508", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "5.6", "", "", "0.14", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC153", "", "", "", "", "For H=0, 3-(BEDT-TTF)2Cu(CF3)4(TCE)", "", "BEDT-TTF", "13.169", "38.031", "8.5388", "", "", "", "4", "", "", "0", "", "", "", "-25", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "plate-like crystal.", "", "", "A new 9 K superconducting organic salt composed of the bis(ethylenedithio)tertrathiafulvalene (ET) electron-donor molecule and the tetrakis(trifluoromethyl)cuprate(III) anion[Cu(CF3)4]-", "1994", "", "", "Physica C (1994) 378-384", "A.S.Komosa,C.A.Achenbach,D.Naumann,H.H.Wang,J.A.Fendrich,J.A.Schlueter,J.D.Dudek,J.E.Schirber,J.M.Williams,K.D.Carlson,P.M.Keane,T.Roy,U.Geiser,U.Welp,W.R.Bayless,w.-K.Kwok", "Organic", "" ] }, { "id": "164", "line_start": 154, "line_end": 154, "sha256": "d7189f274717de82203c66d14f6ab87f9b7fa934cc281a8030d8b6527b7d90a1", "values": [ "164", "PHC2300378", "Cu(CF3)4(TCE)", "kappa-(BEDT-TTF)2Cu(CF3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "9.2", "", "", "0", "", "", "", "-30", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "needle-like crystal. 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SP-heat measured for 1.9. vol = 1776.3 A3. Tc(on) = 9.5 K.", "", "", "A new organic superconductor, ramda-(BEDT-TSF)2GaCl4", "1993", "O-197", "", "Chem. Lett., 1993(1993)1559", "H.Kobayashi,et al.", "", "" ] }, { "id": "198", "line_start": 184, "line_end": 184, "sha256": "06b0f79589f9293bd850bc0592b8939dfc4921b7b78c80461f3b2a9f61e442c8", "values": [ "198", "CL19870507", "I3", "kappa-(BEDT-TTF)2I3", "", "BEDT-TTF", "16.387", "8.466", "12.832", "", "108.56", "", "3.6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "A new ambient -pressure superconductor, kappa-(BEDT-TTF)2I3", "1987", "O-198", "", "Chem. Lett., 1987(1987)507", "R.Kato,et al", "", "" ] }, { "id": "199", "line_start": 185, "line_end": 185, "sha256": "65c9d79994cd8702969aa84b2e92bd0d56dd2cd3e5d283928fed70c8626e9618", "values": [ "199", "MOL1190361", "I3", "beta-(BEDT-TTF)2I3", "", "BEDT-TTF", "6.609", "9.083", "15.267", "85.63", "95.62", "70.22", "1.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G= P1<->. vol = 852 A3.", "", "", "", "1985", "O-199", "", "Mol.Cryst.Liq.Cryst., 119(1985)361", "R.P.Shibaeva,et al", "", "" ] }, { "id": "200", "line_start": 186, "line_end": 186, "sha256": "cee474520938e62a92760ed2a62f40d9373191df9aa4f318314820a5209f0708", "values": [ "200", "MOL1190361", "(I3)2.5", "gamma-(BEDT-TTF)2(I3)2.5", "", "BEDT-TTF", "13.76", "14.73", "33.61", "90", "90", "90", "2.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G= Pbnm. vol = 6812 A3.", "", "", "", "1985", "O-199", "", "Mol.Cryst.Liq.Cryst., 119(1985)361", "R.P.Shibaeva,et al", "", "" ] }, { "id": "201", "line_start": 187, "line_end": 187, "sha256": "492ec853fca997338f28d42d3666dd64500e959c2b9519c88415f5aded429f77", "values": [ "201", "CL19860789", "I3", "theta-(BEDT-TTF)2I3", "", "BEDT-TTF", "10.076", "33.853", "4.964", "", "", "", "3.6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G= Pnma. vol = 1693 A3. system: pseudo orthorhombic", "", "", "A new molecular superconductor, (BEDT-TTF)2(I3)1-x(AuI2)x (x<0.02)", "1986", "O-201", "", "Chem. Lett., 1986(1986)789", "H.Kobayashi,et al", "", "" ] }, { "id": "202", "line_start": 188, "line_end": 188, "sha256": "8ec30b5b2ea91e8359a6a2baca3586ae70ad9a5a96abe53c7b8391bd58405dbd", "values": [ "202", "ACS1189996", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "", "BEDT-TTF", "", "", "", "", "", "", "5.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Superconductivity at 5.2 K in an electron donor radical salt of bis(ethylenedithio)tetrathiafulvalene(BEDT-TTF) with the novel polyfluorinated organic anion SF5CH2CF2SO3-", "1996", "O-202", "", "J.Am.Chem.Soc., 118(1996)9996", "H.H.Wang,J.A.Schlueter,Urs Geiser,et al", "", "" ] }, { "id": "203", "line_start": 189, "line_end": 189, "sha256": "7c0b740bb0c246ef3b76eda688bf19a782685a5534f8b057be03e724526b9c6b", "values": [ "203", "AC12111243", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "1.8", "1.8", "0.3", "0.3", "", "", "", "-5", "", "", "", "", "", "", "", "", "", "", "", "", "8", "", "", "", "", "", "ramda-type (triclinic)", "", "", "Pressure-induced superconducting transition of ramda-(BETS)2FeCl4 with pai-d coupled antiferromagnetic insulating ground state at ambient pressure [BETS=bis(ethylenedithio)tetraselenafulvalene]", "1999", "O-203", "", "J.Am.Chem.Soc., 121(1999)11243", "A.Kobayashi,E.Ojima,H.Fujiwara,H.Kobayashi,H.Tanaka,K.Kato,P.Cassoux,T.Adachi", "", "" ] }, { "id": "204", "line_start": 190, "line_end": 190, "sha256": "ef93b9c5dc9357066d7f931e6d5d6759eb56f4f12b3960ec543be9e3f854b13c", "values": [ "204", "ACS1215581", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-5.5", "2.5", "", "", "", "", "", "Both for H// and H#, SUS obeys C-W law (100-300 K). Hc2(0.6K) = 70 Oe.", "", "", "Antiferromagnetic organic metal exhibiting superconducting transition, kappa-(BETS)2FeBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene]", "1999", "O-204", "", "J.Am.Chem.Soc., 121(1999)5581", "A.Kobayashi,E.Ojima,H.Fujiwara,H.Kobayashi,H.Tanaka,K.Kato,M.Tokumoto,P.Cassoux", "", "" ] }, { "id": "205", "line_start": 191, "line_end": 191, "sha256": "d10a396b7b2ca5f33f17b1541a974b12b68fbc910100bbb635ee5ec175e96808", "values": [ "205", "INO0233839", "IBr2", "beta-(BEDT-TTF)2IBr2", "", "BEDT-TTF", "", "", "", "", "", "", "2.7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "meta stable phase has Tc=4.22 K.", "", "", "Ambient-pressure superconductivity at 2.7 K and higher temperatures in derivatives of (BEDT-TTF)2IBe2: Synthesis, structure, and detection of superconductivity", "1984", "O-205", "", "Inorg.Chem., 23(1984)3839", "F.Behroozi,G.W.Crabtree,H.H.Wang,J.M.Williams,K.D.Carlson,L.M.Sowa,L.N.Hall,M.A.Reno,P.T.Copps,T.J.Emge", "", "" ] }, { "id": "206", "line_start": 192, "line_end": 192, "sha256": "0846b0ca6fe94704ce46fb220165c974cf19abcee9f51ab826765a07450c46c0", "values": [ "206", "INO0242465", "AuI2", "beta-(BEDT-TTF)2AuI2", "", "BEDT-TTF", "", "", "", "", "", "", "4.98", "", "", "0", "", "", "", "10", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "volume =828.7 A3.", "", "", "Ambient-pressure superconductivity at the highest temperature (5K) observed in an organic system: beta-(BEDT-TTF)2AuI2", "1985", "O-206", "", "Inorg.Chem., 24(1985)2465", "G.W.Crabtree,H.H.Wang,J.E.Schirber,J.F.Kwak,J.M.Williams,K.D.Carlson,K.S.Webb,L.J.Azevedo,L.Nunez,M.A.Firestone,M.A.Reno,Urs Geiser", "", "" ] }, { "id": "207", "line_start": 193, "line_end": 193, "sha256": "180d6b631af3b0e892cac997b196b4bed7eda2f6233d9ee801b2ed97b7a24e50", "values": [ "207", "SSC0800843", "Cu[N(CN)2]CN", "kappa-(BEDT-TTF)2Cu[N(CN)2]CN", "", "BEDT-TTF", "", "", "", "", "", "", "10.7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "NEW AMBIENT-PRESSURE ORGANIC SUPERCONDUCTORS BASED ON BEDT-TTF,CU,N(CN)2 AND CN WITH TC=10.7K AND 3.8K", "1991", "", "DEPARTMENT OF CHEMISTRY,FACULTY OF SCIENCE,KYOTO UNIVERSITY,SAKYO-KU,KYOTO 606-01,JAPAN", "SOLID STATE COMMUN.,80(1991)843", "G.Saito,H.Ito,H.Yamochi,K.Sakaguchi,M.Kusunoki,N.Matsukawa,T.Ishiguro,T.Komatsu,T.Nakamura", "", "" ] }, { "id": "208", "line_start": 194, "line_end": 194, "sha256": "2c3671e07349f90af1903554015d8ead96c29d643492814e071bed72cedf158c", "values": [ "208", "SSC0800843", "Cu[N(CN)2]CN:2H2O", "kappa-(BEDT-TTF)2Cu[N(CN)2]CN:2H2O", "", "BEDT-TTF", "", "", "", "", "", "", "3.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "NEW AMBIENT-PRESSURE ORGANIC SUPERCONDUCTORS BASED ON BEDT-TTF,CU,N(CN)2 AND CN WITH TC=10.7K AND 3.8K", "1991", "", "DEPARTMENT OF CHEMISTRY,FACULTY OF SCIENCE,KYOTO UNIVERSITY,SAKYO-KU,KYOTO 606-01,JAPAN", "SOLID STATE COMMUN.,80(1991)843", "G.Saito,H.Ito,H.Yamochi,K.Sakaguchi,M.Kusunoki,N.Matsukawa,T.Ishiguro,T.Komatsu,T.Nakamura", "", "" ] }, { "id": "209", "line_start": 195, "line_end": 195, "sha256": "cb8b70681052abf2ec42db20402b143196b556c4b3b741cd9d64fd437a319118", "values": [ "209", "SSC0800411", "Pt(CN)4:H2O", "(BEDT-TTF)4Pt(CN)4:H2O", "", "BEDT-TTF", "11.514", "16.704", "9.563", "91.22", "112.3", "75.48", "", "2", "0.65", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "triclinic. space-G=P1(-). M-I transition at 120 K(P=0).", "", "", "SUKPERCONDUCTIVITY IN (BEDT-TTF)4PT(CN)4H2O", "1991", "", "INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,MUTSUNO NAGOYA 456,JAPAN", "SOLID STATE COMMUN.,80(1991)411", "H.Inokuchi,H.Mori,I.Hirabayashi,S.Tanaka,T.Mori,Y.Murayama", "", "" ] }, { "id": "210", "line_start": 196, "line_end": 196, "sha256": "9bc4a2c83d223bd155cb934e1d63cd6c709c393d0e76bcd9970cc2d96256ff1c", "values": [ "210", "SSC0760035", "Ag(CN)2:H2O", "kappa-(BEDT-TTF)2Ag(CN)2:H2O", "", "BEDT-TTF", "16.053", "8.635", "12.661", "", "109.27", "", "5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "monoclinic.", "", "", "A NEW AMBIENT-PRESSURE ORGANIC SUPERCONDUCTOR,K-(BEDT-TTF)2AG(CN)2H2O (TC=5.0 K)", "1990", "", "", "SOLID STATE COMMUN,76(1990)35", "H.Inokuchi,H.Mori,I.Hirabayashi,S.Tanaka,T.Mori", "", "" ] }, { "id": "211", "line_start": 197, "line_end": 197, "sha256": "f885dd9dd869c3399643bbf734a39db7184c59ce35aefd6a5daa2e6fac1f7b8c", "values": [ "211", "SSC0641279", "I3", "kappa-(BEDT-TTF)2I3", "", "BEDT-TTF", "16.39", "8.47", "12.83", "", "108.56", "", "3.6", "", "", "0", "", "", "", "", "", "", "6.8", "", "359", "", "", "", "", "", "", "", "", "", "", "", "", "", "monoclinic. space-G=P2<1>/C. RRR=57.3. I//bc-plane(conduction plane). Hc2(n)=0.256T. COHERE(n) = 13.5 A. For I(n), Tc=3.55 K and RRR=385.", "", "", "NEW ORGANIC SUPERCONDUCTORS K-AND (BEDT-TTF)2I3: TRANSPORTPROPERTY", "1987", "", "", "SOLID STATE COMMUN.,64(1987)1279", "A.Kobayashi,H.Kobayashi,K.Kajita,R.Kato,S.Moriyama,W.Sasaki,Y.Nishio", "", "" ] }, { "id": "212", "line_start": 198, "line_end": 198, "sha256": "7187456c769156e09547cbd8f3de5fb40db2a10e38c840ab0472cc4aabd2dff7", "values": [ "212", "SSC0641279", "I3", "theta-(BEDT-TTF)2I3", "", "BEDT-TTF", "10.076", "33.85", "4.964", "", "", "", "3.6", "", "", "0", "", "", "", "", "", "", "0.228", "", "380", "", "", "", "", "", "", "", "", "", "", "", "", "", "orthorhombic. RRR=181. I//ac-plane(conduction plane). Hc2(0) in DB shows Hc2(n).", "", "", "NEW ORGANIC SUPERCONDUCTORS K-AND (BEDT-TTF)2I3: TRANSPORTPROPERTY", "1987", "", "", "SOLID STATE COMMUN.,64(1987)1279", "A.Kobayashi,H.Kobayashi,K.Kajita,R.Kato,S.Moriyama,W.Sasaki,Y.Nishio", "", "" ] }, { "id": "213", "line_start": 199, "line_end": 199, "sha256": "91af2d86e06613b7205af590ff1225f0a1f0ecff3311d6fb3fa54144473096e4", "values": [ "213", "SYN1140243", "HgCl3:TCE", "(BEDT-TTF)2HgCl3:TCE", "", "BEDT-TTF", "39.236", "6.676", "14.881", "90", "95.589", "90", "", "", "", "", "", "", "", "", "154", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC down to 154 K. semiconductor like (activation energy = 0.308 eV). density = 2.071 g/cm3.", "", "", "Structure and electrical conductivity of (BEDT-TTF)2HgCl3:TCE", "2000", "O-213", "University of Jinan, China", "Synth.Metals, 114(2000)243", "Chen Shen-Hao,Fang Qi,Jiang Min-Hua,Liu Zhi,Yu Wen-Tao,Zhang Bin,Zhang Jin-Biao,Zhu Dao-Ben", "", "" ] }, { "id": "214", "line_start": 200, "line_end": 200, "sha256": "ea0d7a985d5d88652b92c9d3a9df67712108b922d9f68dd5fe24a45f592bfdb9", "values": [ "214", "PHC3880595", "Hg2.89Br8", "kappa-(BEDT-TTF)4Hg2.89Br8", "", "BEDT-TTF", "", "", "", "", "", "", "4.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "20", "7", "", "", "", "", "", "", "", "Debye-T = 7 K for 3-D and 150 K for 1-D analysis using Tarasov's model.", "", "", "Low-temperature heat capacity measurements of kappa-(BEDT-TTF)4Hg2.89Br8", "2003", "O-214", "Research Center for Molecular Thermodynamics, Osaka-University,Toyonaka, Osaka, Japan", "Physica C, 388-389(2003)595", "A.Naito,H.Taniguchi,K.Kanoda,K.Saito,M.Sorai,Y.Nakazawa", "", "" ] }, { "id": "215", "line_start": 201, "line_end": 201, "sha256": "7f24ce7718d46bd0ffb8899a778c3442500672a2c8215c8c88bc8873b2956510", "values": [ "215", "SSC0820177", "Pd(CN)4H2O", "(BEDT-TTF)4Pd(CN)4H2O", "", "BEDT-TTF", "11.529", "16.685", "9.562", "91.32", "112.29", "75.63", "1.2", "", "", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-Semicond transition at 250 K. thermopower also measured.", "", "", "STRUCTURAL AND PHYSICAL PROPERTIES OF A NEW ORGANIC SUPERCONDUCTOR,(BEDT-TTF)4PD(CN)4H2O", "1992", "", "", "SOLID STATE COMMUN.82(1992)177", "H.Inokuchi,H.Mori,I.Hirabayashi,K.Kato,S.Tanaka,T.Mori,Y.Murayama", "", "" ] }, { "id": "216", "line_start": 202, "line_end": 202, "sha256": "e5b100c277f80801bc684363a014303e9db16d068a8cb77ea5b18b1bb256ba99", "values": [ "216", "P071024531", "SbF6", "beta-(BDA-TTP)2SbF6", "2", "BDA-TTP", "", "", "", "", "", "", "6.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC216", "", "", "", "", "Thermal conductivity (THC) was measured for various H. Hc2(T) determined from THC and R measurements.", "OHC216.dat", "", "Thermal conductivity of layered organic superconductor beta-(BDA-TTP)2SbF6 in a parallel magnetic field: Anomalous effect of coreless vortices", "2005", "", "Department of Physics, Kyoto University, Kyoto 606-8502, Japan", "Phys.Rev.B, 71(2005)024531", "J.Yamada,M.A.Tanatar,T.Ishiguro,T.Toita", "", "" ] }, { "id": "217", "line_start": 203, "line_end": 203, "sha256": "338dd0057b7ab4fb2e3fa8b29007e5219bf3e2cb82d0d0b2c13ca3f6a27a9698", "values": [ "217", "PHB2940427", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2", "BEDT-TTF", "", "", "", "", "", "", "11.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC217", "", "", "", "", "Hc2//conduction plane from resistive transition. out-of-plane resistivity.", "OHC217.dat", "", "Upper critical field of kappa-(ET)2Cu[N(CN)2]Br under parallel magnetic fields", "2001", "", "", "Physica B, 294-295(2001)427", "A.Ayari,A.E.Kovalev,E.Ohmichi,G.Saito,H.Yamochi,P.Monceau,S.Kamiya,T.Ishiguro,Y.Shimojo", "", "" ] }, { "id": "218", "line_start": 204, "line_end": 204, "sha256": "f4aa71f18308e26f3f4a928a77995d8d51cb880e0c3181a9b14d1d216038b08b", "values": [ "218", "PR06111739", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.75", "", "", "0", "", "", "", "3.9", "", "", "10.4", "", "7.9", "", "", "", "", "", "", "", "", "OHC218", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, a-axis.", "OHC218.dat", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "219", "line_start": 205, "line_end": 205, "sha256": "ef6b683f50e96067435fcc89341ab2abd92d42f29572c571b2fa6c77d12449c6", "values": [ "219", "PR06111739", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.75", "", "", "0", "", "", "", "39", "", "", "10.4", "", "7.9", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, b-axis.", "", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "220", "line_start": 206, "line_end": 206, "sha256": "49ec75330392295bf15ce021e54d098ca24d76e95390d4b2eb0e07194f180984", "values": [ "220", "PR06111739", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "2", "BEDT-TTF", "", "", "", "", "", "", "4.6", "", "", "0", "", "", "", "-59", "", "", "1.4", "", "144", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, c-axis.", "", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "221", "line_start": 207, "line_end": 207, "sha256": "44020678ca308d02f797750eb896144baa9d5a54aab26177a1434820e571f671", "values": [ "221", "PR06111739", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.95", "", "", "0", "", "", "", "34.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, c-axis(in plane).", "", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "222", "line_start": 208, "line_end": 208, "sha256": "1e3f0e5d825ba814bfe0f9a0183924f9be1ed73234964b2cfd6ab6fea24613ef", "values": [ "222", "PR06111739", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.95", "", "", "0", "", "", "", "-1.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, b-axis(in plane).", "", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "223", "line_start": 209, "line_end": 209, "sha256": "fea0d7f041eb321241d06d81e72c2b368adabd201d0a24f09ef8025c2dd52dfd", "values": [ "223", "PR06111739", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.95", "", "", "0", "", "", "", "-62", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "thermal expansion coeff. were measured for 3 directions. uniaxial pressure, a*-axis(out-of-plane).", "", "", "Comparative thermal-expansion study of beta ''-(ET)2SF5CH2CF2SO3 and kappa -(ET)2Cu(NCS)2: Uniaxial pressure coefficients of Tc and upper critical fields", "2000", "", "", "Phys.Rev.B, 61(2000)11739", "A.M.Kini,F.Steglich,G.L.Gard,J.A.Schlueter,J.Mohtasham,J.Muller,M.Lang,N.Toyota,R.W.Winter,T.Sasaki,U.Geiser", "", "" ] }, { "id": "224", "line_start": 210, "line_end": 210, "sha256": "a5ea75e72b115ac3561f13bacdae51c2dec69e1e18c53992c671f6e432e8bc0b", "values": [ "224", "JPS0710717", "SbF6", "beta-(BDA-TTP)2SbF6", "", "BDA-TTP", "", "", "", "", "", "", "6.31", "", "", "0", "", "", "", "", "", "0.5", "12", "", "105", "6800", "260", "", "", "33", "", "", "", "", "", "", "", "", "H//conduction plane. thermodynamic Hc(0)=33 mT. (delta-C/gamma*Tc) = 1.1", "", "", "Superconductivity of Layered Organic Compound beta-(BDA-TTP)2SbF6, Where BDA-TTP is 2,5-Bis(1,3-dithian-2-ylidene)-1,3,4,6-tetrathiapentalene", "2002", "", "Physics Department, Kyoto University, Kyoto 606-8", "J.Phys.Soc.Jpn, 71(2002)717", "J.Yamada,T.Ishiguro,T.Toita,Y.Shimojo", "", "" ] }, { "id": "225", "line_start": 211, "line_end": 211, "sha256": "fa4c9813505b72f0a6caa13f6a044bea45e050d865b6952acaa0e76f7145e2e3", "values": [ "225", "JPS0710717", "SbF6", "beta-(BDA-TTP)2SbF6", "", "BDA-TTP", "", "", "", "", "", "", "6.31", "", "", "0", "", "", "", "", "", "1.5", "3", "", "26", "27000", "64", "", "", "", "", "", "", "", "", "", "", "", "H perpendicular to plane.", "", "", "Superconductivity of Layered Organic Compound beta-(BDA-TTP)2SbF6, Where BDA-TTP is 2,5-Bis(1,3-dithian-2-ylidene)-1,3,4,6-tetrathiapentalene", "2002", "", "Physics Department, Kyoto University, Kyoto 606-8", "J.Phys.Soc.Jpn, 71(2002)717", "J.Yamada,T.Ishiguro,T.Toita,Y.Shimojo", "", "" ] }, { "id": "226", "line_start": 212, "line_end": 212, "sha256": "642faa34c89ee14d5bb2f4e6bc64c56087440bb84b34053b1413fc933b11565e", "values": [ "226", "JPS0741529", "I3", "(MDT-ST)(I3)0.417", "2", "MDT-ST", "", "", "25.286", "", "", "", "4.3", "", "", "0", "", "", "", "", "", "", "", "", "278", "", "", "", "", "", "", "", "", "", "", "", "", "", "coherence-L(1.6 K): //a=278, //b=205, //c=25 A. anisotropy (a vs c) = 10 at 1.6 K. lat-c measured at 18.5 K.", "", "", "Anisotropic Three-dimensional Superconductivity of the Incommensurate Organic Superconductor (MDT-ST)(I3)0.417", "2005", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo", "J.Phys.Soc.Jpn, 74(2005)1529", "T.Kawamoto,T.Mori,T.Terashima,S.Uji,A.Takamori,K.Takimiya,T.Otsubo", "", "" ] }, { "id": "227", "line_start": 213, "line_end": 213, "sha256": "7af14b82b62226f324854c1819dd64b527a8ca63f0adef923a9396d6898b8ecc", "values": [ "227", "P071054514", "HgxBr4", "kappa-(BEDT-TTF)2Hg1.445Br4", "2", "BEDT-TTF", "", "", "", "", "", "", "3", "", "", "0", "", "", "", "", "", "", "", "", "70", "", "", "", "", "55", "200", "", "", "", "", "", "", "", "best fit below 2K(gamma=55 mj/mol.K2, beta=32 mj/mol.K4, A=2.6 mj.K/mol. 1D-Debye = 200K, 3D-Debye = 6.5 K.", "", "", "Anomalous enhancement of electronic heat capacity in the organic conductors kappa-(BEDT-TTF)4Hg3-zX8 (X=Br,Cl)", "2005", "", "Department of Chemistry, Tokyo Institute of Technology, O-okayama, Meguro-Ku, Tokyo 152-8551, Japan", "Phys.Rev.B, 71(2005)054514", "A.Naito,Y.Nakazawa,K.Saito,H.Taniguchi,K.Kanoda,M.Sorai", "", "" ] }, { "id": "228", "line_start": 214, "line_end": 214, "sha256": "838fa6bba437c82a26ef9c0018b1336259e60dd28b584a2a69afdaff1291cf4a", "values": [ "228", "P071054514", "HgxBr4", "kappa-(BEDT-TTF)2Hg1.39Cl4", "2", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.4", "", "", "", "", "", "", "", "", "52", "", "", "", "", "", "", "", "", "not SC", "", "", "Anomalous enhancement of electronic heat capacity in the organic conductors kappa-(BEDT-TTF)4Hg3-zX8 (X=Br,Cl)", "2005", "", "Department of Chemistry, Tokyo Institute of Technology, O-okayama, Meguro-Ku, Tokyo 152-8551, Japan", "Phys.Rev.B, 71(2005)054514", "A.Naito,Y.Nakazawa,K.Saito,H.Taniguchi,K.Kanoda,M.Sorai", "", "" ] }, { "id": "229", "line_start": 215, "line_end": 215, "sha256": "90ffa340853eb2bc53995786ca9a403ef18fd0cc212543660339aaf0b4d27ed7", "values": [ "229", "JPC015L669", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTHC229", "", "", "", "", "T-independent thermal conductivity for 120 < T < 300K", "OTHC229.dat", "", "Magnetic field dependent thermal conductivity in the organic superconductor (TMTSF)2ClO4", "1982", "", "", "J.Phys.C: Solid State Phys., 15(1982)L669", "D.Djurek,M.Prester,D.Jerome,K.Bechgaard", "", "" ] }, { "id": "230", "line_start": 216, "line_end": 216, "sha256": "861af0dc44cfdb329d494633211f6c1ef53cb52229c11aff1f1e4a02d5fbee01", "values": [ "230", "P072052510", "PF6", "beta''-(DODHT)2PF6", "2", "DODHT", "", "", "", "", "", "", "2.7", "2.7", "", "1.32", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH230", "", "", "", "", "Tc by dc-resistance. P-T phase diagram in Fig.", "OPH230.dat", "", "Charge ordering and pressure-induced superconductivity in beta''-(DODHT)2PF6", "2005", "", "Graduate School of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennoudai, Tsukuba, Ibaraki 305-8571, Japan", "Phys.Rev.B, 72(2005)052510", "H.Nishikawa,Y.Sato,K.Kikuchi,T.Kodama,I.Ikemoto,J.Yamada,H.Oshio,R.Kondo,S.Kagoshima", "", "" ] }, { "id": "231", "line_start": 217, "line_end": 217, "sha256": "2e85f7aac8e2dcab6ec801875c14ca35daa624dc8c8547904454b8bcf6b48c55", "values": [ "231", "P071172503", "I3", "(MDT-ST)(I3)0.417", "2", "MDT-ST", "3.895", "12.283", "25.286", "90", "90", "90", "4.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTP231", "", "", "", "", "Raman. donor lattice const. measured at 18.5 K. Thermopower along a-axis. anisotropy(RT) = 20.", "OTP231.dat", "", "Structural and transport properties of the incommensurate organic superconductor (MDT-ST)(I3)0.417", "2005", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan", "Phys.Rev.B, 71(2005)172503", "T.Kawamoto,T.Mori,S.Uji,J.Yamaura,H.Kitagawa,A.Takamori,K.Takimiya,T.Otsubo", "", "" ] }, { "id": "232", "line_start": 218, "line_end": 218, "sha256": "968955fe230f825b27eaf42236250d9e2566208d7a9c6c1f0b5e47a3962a75f4", "values": [ "232", "P071212503", "CuCl2", "beta-(DMET)2CuCl2", "2", "DMET", "7.023", "7.586", "14.868", "80.18", "89.31", "70.492", "0.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "ac-resistance, magnetoresistance(MR), Hall effect were measured.", "", "", "Quasi-one-dimensional electronic structure of (DMET)2CuCl2", "2005", "", "Department of Applied Physics, Nagoya University, Chikusa, Nagoya, 464-8603, Japan", "Phys.Rev.B, 71(2005)212503", "H.Ito,D.Suzuki,Y.Yokochi,S.Kuroda,M.Umemiya,H.Miyasaka,K-I.Sugiura,M.Yamashita,H.Tajima", "", "" ] }, { "id": "233", "line_start": 219, "line_end": 219, "sha256": "d75a8725d255af4ab44a5c3136658d6c5f114bb10a98845093486b6aa2135171", "values": [ "233", "P071104525", "(Fe,Ga)Cl4", "ramda-(BETS)2Fe0.45Ga0.55Cl4", "2", "BETS", "", "", "", "", "", "", "6", "", "", "0", "", "", "", "", "", "", "5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "paramag-SC-Antiferro transition as decreasing T. Tc(R=0) = 4.2K.", "", "", "Superconductivity and vortex phases in the two-dimensional organic conductor ramda-(BETS)2FrxGa1-xCl4 (x=0.45)", "2005", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 71(2005)104525", "S.Uji,T.Terashima,Y.Terai,S.Yasuzuka,M.Tokumoto,H.Tanaka,A.Kobayashi,H.Kobayashi", "", "" ] }, { "id": "235", "line_start": 220, "line_end": 220, "sha256": "d782227b2883b44f71804c62c289fbda31759f54e89f087a76c476e0108b5643", "values": [ "235", "P072184505", "FeCl4", "ramda-(BETS)2FeCl4", "3", "BETS", "", "", "", "", "", "", "", "5.5", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "OPH235", "", "", "", "", "H-induced SC. H//ac plane(conducting). Tc(max) at H = 36 T. orbital critical field(Hc2) = 55 T. RRR = 29 .", "OPH235.dat", "", "Magnetic-field-induced superconductivity and phase diagrams of ramda-(BETS)2FeCl4-xBrx", "2005", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 72(2005)184505", "S.Uji,S.Yasuzuka,M.Tokumoto,H.Tanaka,A.Kobayashi,B.Zhang,H.Kobayashi,E.S.Choi,D.Graf,J.S.Brooks", "", "" ] }, { "id": "236", "line_start": 221, "line_end": 221, "sha256": "d81555cfa68dfc4ca977945aa8224c6828fc02f50dbc6aa46f22b9f6de2189c0", "values": [ "236", "P072184505", "FeCl3.6Br0.4", "ramda-(BETS)2FeCl3.6Br0.4", "3", "BETS", "", "", "", "", "", "", "", "2.3", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "OPH236", "", "", "", "", "H-induced SC. H//ac plane(conducting). Tc(max) at H = 31 T. orbital critical field(Hc2) = 140 T. RRR = 6.7 .", "OPH236.dat", "", "Magnetic-field-induced superconductivity and phase diagrams of ramda-(BETS)2FeCl4-xBrx", "2005", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 72(2005)184505", "S.Uji,S.Yasuzuka,M.Tokumoto,H.Tanaka,A.Kobayashi,B.Zhang,H.Kobayashi,E.S.Choi,D.Graf,J.S.Brooks", "", "" ] }, { "id": "237", "line_start": 222, "line_end": 222, "sha256": "3787194726a35b4df81a9bd4630bd79e2a226c6b8622308b0d47a587f97e653c", "values": [ "237", "P072184505", "FeCl3.5Br0.5", "ramda-(BETS)2FeCl3.5Br0.5", "3", "BETS", "", "", "", "", "", "", "", "3", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "OPH237", "", "", "", "", "H-induced SC. H//ac plane(conducting). Tc(max) at H = 33 T. orbital critical field(Hc2) = 110 T. RRR = 7.3.", "OPH237.dat", "", "Magnetic-field-induced superconductivity and phase diagrams of ramda-(BETS)2FeCl4-xBrx", "2005", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 72(2005)184505", "S.Uji,S.Yasuzuka,M.Tokumoto,H.Tanaka,A.Kobayashi,B.Zhang,H.Kobayashi,E.S.Choi,D.Graf,J.S.Brooks", "", "" ] }, { "id": "238", "line_start": 223, "line_end": 223, "sha256": "4c27e08dcafb0b4509b031228439c760e488712c1015a77b3ee76f4727a3ec77", "values": [ "238", "P072184505", "FeCl3.3Br0.7", "ramda-(BETS)2FeCl3.3Br0.7", "3", "BETS", "", "", "", "", "", "", "", "2.6", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "OPH238", "", "", "", "", "H-induced SC. H//ac plane(conducting). Tc(max) at H = 34 T. orbital critical field(Hc2) = 100 T. RRR = 6.6.", "OPH238.dat", "", "Magnetic-field-induced superconductivity and phase diagrams of ramda-(BETS)2FeCl4-xBrx", "2005", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 72(2005)184505", "S.Uji,S.Yasuzuka,M.Tokumoto,H.Tanaka,A.Kobayashi,B.Zhang,H.Kobayashi,E.S.Choi,D.Graf,J.S.Brooks", "", "" ] }, { "id": "239", "line_start": 224, "line_end": 224, "sha256": "e118258913b8a56a64b5d1337d734954df561e62ec8625e2be6c38dd1095cbee", "values": [ "239", "P072174513", "KHg(SCN)4", "alpha-(BEDT-TTF)2KHg(SCN)4", "3", "BEDT-TTF", "", "", "", "", "", "", "0.11", "0.11", "0.25", "0.25", "", "", "", "-0.3", "0", "", "", "", "", "", "", "", "", "", "", "", "", "OHC239", "OPH239", "", "", "", "P-induced SC. I//conducting layer. hydrostatic P. CDW state suppressed completely at Pc and SC state appears. Below Pc, CDW and SC coexist.", "OHC239.dat", "OPH239.dat", "Superconductivity in the charge-density-wave state of the organic metal alpha-(BEDT-TTF)2KHg(SCN)4", "2005", "", "Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, D-85748 Garching, Germany", "Phys.Rev.B, 72(2005)174513", "D.Andres,M.V.Kartsovnik,W.Biberacher,N.Neumaier,E.Schuberth,H.Muller", "", "" ] }, { "id": "240", "line_start": 225, "line_end": 225, "sha256": "657c74f2bd6a6d33937e7e71093495e7278639d7586f05c56e57b9a7e11bc787", "values": [ "240", "JPS0741370", "AuCl2", "beta'-(BEDT-TTF)2AuCl2", "", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "28", "", "", "", "", "", "not SC upto 9.9 GPa. activation energy = 114 meV. Rho(290K) = 27 Ohm.cm", "", "", "High-Pressure Study up to 9.9 GPa of Organic Mott Insulator, beta'-(BEDT-TTF)2AuCl2", "2005", "", "Department of Physics, Faculty of Science, Saitama University, 255 Shimo-Ohkubo, Saitama", "J.Phys.Soc.Jpn, 74(2005)1370", "H.Taniguchi,M.Miyashita,K.Uchiyama,R.Sato,Y.Ishii,K.Satoh,N.Mori,M.Hedo,Y.Uwatoko", "", "" ] }, { "id": "241", "line_start": 226, "line_end": 226, "sha256": "afa2f5615e93d37bc46fc8597a73609478c2d3ebeefc39b170c9485c8a0da5e7", "values": [ "241", "P072014543", "[(H3O)Cr(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Cr(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "6", "", "", "0", "", "", "", "", "", "", "11.8", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ph = C6H5. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 1.7 T. M-I transition(defined as R(min) = 89 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "242", "line_start": 227, "line_end": 227, "sha256": "abc9d3395219ed60d1bfb39bdb5cbdabdeab3da93674a40ca59151fd70f56137", "values": [ "242", "P072014543", "[(H3O)Cr(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Cr(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "5.3", "", "", "0", "", "", "", "", "", "", "18.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ph = C6H5. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 2.2 T. M-I transition(defined as R(min) = 94 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "243", "line_start": 228, "line_end": 228, "sha256": "b2086074d540c3f2b5a12e698185ce61a4271ae17e13d7d0d93bb03cbe7f0ca3", "values": [ "243", "P072014543", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "7", "", "", "0", "", "", "", "", "", "", "33.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ph = C6H5. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 5.2 T. M-I transition(defined as R(min) = 68 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "244", "line_start": 229, "line_end": 229, "sha256": "5efaca681bef0dc256459a73f14d3f85f5d62397a91238977a94ddd3e524d82b", "values": [ "244", "P072014543", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "", "", "", "", "", "", "32", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ph = C6H5. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 6.5 T. M-I transition(defined as R(min) = 69 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "245", "line_start": 230, "line_end": 230, "sha256": "cf504dac9b82aea0597963e2703124bf65ca4b0bfb220eae0921a2a4a7cd1284", "values": [ "245", "P072014543", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "", "", "", "", "", "", "31", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ph = C6H5. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 5.9 T.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "246", "line_start": 231, "line_end": 231, "sha256": "72694828e00da3dfab92f4a978cd999e06d414698c9a2c477e37c32e0cb6f5b6", "values": [ "246", "P072014543", "[(H3O)Fe(C2O4)3]:PhCN", "beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhCN", "", "BEDT-TTF", "", "", "", "", "", "", "6.5", "", "", "0", "", "", "", "", "", "", "17.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "PhCN=C6H5CN. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 3.3 T. M-I transition(defined as R(min) = 154 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "247", "line_start": 232, "line_end": 232, "sha256": "95464098869b5aec7f05d1416dfa25da19b744091097f23b618d74edf5118dcd", "values": [ "247", "P072014543", "[(H3O)Fe(C2O4)3]:PhCN", "beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhCN", "", "BEDT-TTF", "", "", "", "", "", "", "4.7", "", "", "0", "", "", "", "", "", "", "18.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "PhCN=C6H5CN. Tc defined as Tc(on). Hc2 at 0.5 K. nHc2(0.5K) = 3.6 T. M-I transition(defined as R(min) = 124 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "248", "line_start": 233, "line_end": 233, "sha256": "f370152b4f7e813171e71c1201b1b65af3b53cffdfc1297dd6b5a6e79b457c68", "values": [ "248", "P072014543", "[(H3O)Fe(C2O4)3]:PhCN", "beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhCN", "", "BEDT-TTF", "", "", "", "", "", "", "6", "", "", "0", "", "", "", "", "", "", "16", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "PhCN=C6H5CN. Tc defined as Tc(on). Hc2 at 0.5 K.", "", "", "Robust superconducting state in the low-quasiparticle-density organic metals beta''-(BEDT-TTF)4[(H3O)M(C2O4)3]/Y: Superconductivity due to proximity to a charge-ordered state", "2005", "", "Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.B, 72(2005)014543", "A.F.Bangura,A.I.Coldea,J.Singleton,A.Ardavan,A.Akutsu-Sato,H.Akutsu,S.S.Turner,P.Day,T.Yamamoto,K.Yakushi", "", "" ] }, { "id": "249", "line_start": 234, "line_end": 234, "sha256": "e8f96f5b3f2a80fd73a8bf3ad993d20d7ee41d567f5b6665d19467794115167f", "values": [ "249", "JPS0720468", "ICl2", "beta'-(BEDT-TTF)2ICl2", "3", "BEDT-TTF", "", "", "", "", "", "", "14.2", "14.2", "8.2", "7", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "22", "OTC249", "", "Tc(P)", "", "", "Tc defined as Tc(on). resistive transition. crystals by galvanostatic anodic oxidation using (n-Bu)4NICl2 in tetrahydrofuran.", "OTC249.dat", "", "Superconductivity at 14.2K in Layered Organics under Extreme Pressure", "2003", "", "Department of Physics, Faculty of Science, Saitama University, Shimo-Ohkubo 255, Saitama, Japan", "J.Phys.Soc.Jpn, 72(2003)468", "H.Okamoto,H.Taniguchi,K.Kanoda,K.Miyagawa,K.Satoh,K.Uchiyama,M.Hedo,M.Miyashita,N.Mori,Y.Uwatoko", "", "" ] }, { "id": "250", "line_start": 235, "line_end": 235, "sha256": "d67e489bf95266c35baf799585ee97058ce91f8cddcece8903ca314eaa29b216", "values": [ "250", "P067014516", "FSO3", "(TMTSF)2FSO3", "3", "TMTSF", "", "", "", "", "", "", "3.2", "3.2", "0.48", "0.48", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC250", "", "", "", "", "Thermoelectric power s(295K) = 25.3 uV/K. (ds/dP) = 0.227 uV/K/kbar at 295 K.", "OTC250.dat", "", "Refinement of the pressure-temperature phase diagram of the organic superconductor with asymmetric anions (TMTSF)2FSO3", "2003", "", "Department of Physics, Ewha Womans University, Seoul 120-750, South Korea", "Phys.Rev.B, 67(2003)014516", "Y.J.Jo,E.S.Choi,Haevong Kang,W.Kang,I.S.Seo,O.H.Chung", "", "" ] }, { "id": "251", "line_start": 236, "line_end": 236, "sha256": "40821a933f260d67a623c1fe92910c31ac2e0a8c0cfbd7dafdb8592022335c06", "values": [ "251", "SYN1330011", "BF4", "(TMTTF)2BF4", "3", "TMTTF", "", "", "", "", "", "", "1.38", "", "3.75", "3.35", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "From Mott insulator to superconductivity in (TMTTF)2BF4: high pressure transport measurements", "2003", "", "Laboratoire de Physique des Solides, Universite Paris-Sud, 91405 Orsay, France", "Synth.Met., 133-134(2003)11", "P.Auban-Senzier,C.Pasquier,D.Jerome,C.Carcel,J.M.Fabre", "", "" ] }, { "id": "252", "line_start": 237, "line_end": 237, "sha256": "85aa56185c0dd8ff0215403535fb905971d2384edbbe737df4becb85fa65c0f5", "values": [ "252", "JPC013L089", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "2.2", "2.2", "4.73", "4.35", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH252", "", "", "", "", "Tc defined as Tc(on). Hc2(T)//c-axis was measured. SC region: 4 < P <7 GPa.", "OPH252.dat", "", "From spin-Peierls to superconductivity: (TMTTF)2PF6 under high pressure", "2001", "", "DPMC, Universite de Geneve, Quai E-Ansermet 24, 1211 Geneva 4, Switzerland", "J.Phys.:Condens.Matter, 13(2001)L89", "D.Jaccard,H.Wilhelm,D.Jerome,J.Moser,C.Carcel,J.M.Fabre", "", "" ] }, { "id": "253", "line_start": 238, "line_end": 238, "sha256": "93e9d5e1bbb3bb894ccdc95253ad16b05b7f986ec95e47a7588fd023578435c7", "values": [ "253", "SYN1330239", "Cu(NCS)2", "kappa-(d8-(BEDT-TTF))2Cu(SCN)2", "3", "BEDT-TTF", "", "", "", "", "", "", "12", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC253", "", "", "", "", "deutrated sample. Tc decreases with increasing P. Tc(P=0.25 GPa) = 0 K.", "OTC253.dat", "", "Study of magnetoresistance under hydrostatic pressure in the deuterated organic superconductor d8-kappa-(BEDT-TTF)2Cu(SCN)2", "2003", "", "Clarendon Laboratory, Oxford University, Parks Road, Oxford OX1 3PU, UK", "Synth.Met., 133-134(2003)239", "T.Biggs,D.J.Bakker,A.-K.Klehe,J.A.Symington,J.Singleton,T.Sasaki,M.Kurmoo", "", "" ] }, { "id": "254", "line_start": 239, "line_end": 239, "sha256": "c91b32be03301eda03d152d5f99e32f69495f8843d44ae98332d780cc32b8b51", "values": [ "254", "SYN1330181", "Au(CN)4", "theta-(DIETS)2[Au(CN)4]", "3", "DIETS", "", "", "", "", "", "", "8", "", "", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC under uniaxial pressure along c-axis. not SC under hydrostatic pressure upto 18 kbar. M-I transition of Au(CN)4 salt at 226 K under ambient pressure.", "", "", "Supramolecular organic conductor theta-(DIETS)2[Au(CN)4]: unique crystal structure and superconductivity under uniaxial strain (DIETS = diiodo(ethylenedithio)diselenadithiafulvalene)", "2003", "", "RIKEN, Wako, Saitama 351-0198, Japan", "Synth.Met., 133-134(2003)181", "T.Imakubo,N.Tajima,M.Tamura,R.Kato,Y.Nishio,K.Kajita", "", "" ] }, { "id": "255", "line_start": 240, "line_end": 240, "sha256": "c7d0f43fb16de036e23a50525a69dfd878d0a43627494638a5276734a43e227b", "values": [ "255", "SYN1330219", "GaCl4", "ramda-(BETS)2GaCl4", "3", "BETS", "", "", "", "", "", "", "4.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "14.4", "197", "", "", "", "", "", "", "", "(dC/gamma*Tc) = 1.37. lattice term coeffic. = 14.5 mJ/mol.K4.", "", "", "Specific heat of organic superconductor ramda-(BEDT-TSF)2GaCl4", "2003", "", "Physics Department, Graduate School of Science, Tohoku University, Sendai 980-8578, Japan", "Synth.Met., 133-134(2003)219", "Y.Ishizaki,H.Uozaki,H.Tsuchiya,Y.Abe,E.Negishi,H.Matsui,S.Endo,N.Toyota", "", "" ] }, { "id": "256", "line_start": 241, "line_end": 241, "sha256": "d9096d6c3ce1990ffa7923be548d57bb4978b0dafd0bad4c22fae0200eeb624c", "values": [ "256", "ACS1230306", "4-Feb", "kappa-(BETS)2FeBr4", "3", "BETS", "", "", "", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-5.5", "2.5", "OTC256", "", "", "", "", "lattice const., a,b,c(T) were measured. 3D-ordering of Fe-spins.magnetic easy axis: a-axis. Hc2(a,b,c-axis) were measured.", "OTC256.dat", "", "A novel antiferromagnetic organic superconductor kappa-(BETS)2FeBr4 ", "2001", "", "", "J.Am.Chem.Soc., 123(2001)306", "A.Kobayashi,B.Zh.Narymbetov,E.Fujiwara,H.Fujiwara,H.Kobayashi,K.Kato,M.Tokumoto,P.Cassoux,Y.Nakazawa", "", "" ] }, { "id": "257", "line_start": 242, "line_end": 242, "sha256": "b769e9ac8f96b270ee5e8e4318e5745453b2c547a2f4a827808c37caaa8fdd62", "values": [ "257", "CS11912392", "Fe0.55Ga0.45Cl4", "ramda-(BETS)2Fe0.55Ga0.45Cl4", "3", "BETS", "", "", "", "", "", "", "5.4", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "resistivity restored below Tc. T(M-I) at 2.3 K. Tc and T(M-I) show sample dependency. resistivity maximum at about 100 K.", "", "", "Superconductor-to-Insulator Transition in an Organic Metal Incorporating Magnetic Anions: ramda-(BETS)2(FexGa1-x)Cl4 [BETS = bis(ethylenedithio)tetraselenafulvalene; x = 0.55 and 0.43]", "1997", "", "Institute for Molecular Science,Okazaki, Aichi 444, Japan", "J.Am.Chem.Soc., 119(1997)12392", "H.Kobayashi,A.Sato,E.Arai,H.Akutsu,A.Kobayashi,P.Cassoux", "", "" ] }, { "id": "258", "line_start": 243, "line_end": 243, "sha256": "050219413e8296306a3ac82f5b1c8e079715d8c6c1e7c93a1318f809bd837d8a", "values": [ "258", "PR05608526", "GaBr1.5Cl2.5", "ramda-(BETS)2GaBr1.5Cl2.5", "3", "BETS", "", "", "", "", "", "", "9.7", "9.7", "0.3", "0.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC258", "", "", "", "", "P-induced SC", "OTC258.dat", "", "Electric and magnetic properties and phase diagram of a series of organic superconductors ramda-BETS2GaXzY4-z : BETS = bis(ethylenedithiotetraselenafulvalene; X,Y = F, Cl, Br; 0-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K", "1990", "", "", "Inorg.Chem., 29(1990)1599", "M.A.Beno,H.H.Wang,A.M.Kini,K.D.Carlson,U.Geiser,W.K.Kwok,J.E.Thompson,J.M.Williams,J.Ren,M.H.Whangbo", "", "" ] }, { "id": "265", "line_start": 250, "line_end": 250, "sha256": "8240e3811e8d8f44160e158698b6e5246190888d34b5ac123dd282958138824b", "values": [ "265", "INO0293272", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "", "BEDT-TTF", "12.977", "29.979", "8.48", "", "", "", "12.5", "12.5", "0.03", "0.03", "", "", "", "-34", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G = Pnma. semicon-semicon transition at 42K. not SC down to 0.6K under ambient P.", "", "", "From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, kappa-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K)", "1990", "", "", "Inorg.Chem., 29(1990)3274", "J.M.Williams,A.M.Kini,H.H.Wang,K.D.Carlson,U.Geiser,L.K.Montgomery,G.J.Pyrka,D.M.Watkins,J.M.Kommers,S.J.Boryschuk,A.V.Strieby Crouch,W.K.Kwok,J.E..Schirber,D.L.Overmyer,D.Jung,M.H.Whangbo", "", "" ] }, { "id": "266", "line_start": 251, "line_end": 251, "sha256": "8e3a4b3fb289fc693c743c756efa38daa35f06ede7131d0545f375ea2df55dcf", "values": [ "266", "SSC0800191", "ReO4:(H2O)", "(BEDO-TTF)2ReO4:(H2O)", "", "BEDO-TTF", "12.16", "34.05", "8.091", "", "123.44", "", "0.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "monoclinic phase. Tc by susceptibility. Resistive Tc(on) = 2.5 K. Three phase transitions at 213K, 90K, 35K.", "", "", "(BEDO-TTF)2REO4(H2O): A NEW ORGANIC SUPERCONDUCTOR+", "1991", "", "3.PHYSIKALISCHES INSTITUT DER UNIVERSITAT STUTTGART,PFAFFENWALDRING 57,7000 STUTTGART 80,GERMANY", "SOLID STATE COMMUN.,80(1991)191", "B.NEBER,D.SCHWEITZER,H.J.KELLER,H.W.HELBERG,I.HEINEN,K.WINZER,S.KAHLICH,SONG EN LAN", "", "" ] }, { "id": "267", "line_start": 252, "line_end": 252, "sha256": "06be3913760424965f529a61c277bf41bde52df1d2b59c757d8d39338dbd2a1e", "values": [ "267", "JPS0740412", "Me4Sb", "beta'-Me4Sb[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "8.4", "8.4", "0.45", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for hydrostatic-P (upto 15 kbar) and c*-axis pressure.", "", "", "Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)", "2005", "", "Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan", "J.Phys.Soc.Jpn, 74(2005)412", "A.Tajima,A.Nakao,R.Kato", "", "" ] }, { "id": "268", "line_start": 253, "line_end": 253, "sha256": "4defc10e585aa66aa7a9fcda86e3d63a78ab8641c7e4910e367a1fd62001af77", "values": [ "268", "JPS0740412", "Me2Et2P", "beta'-Me2Et2P[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "6.1", "6.1", "0.45", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. Et=C2H5. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for a-axis pressure.", "", "", "Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)", "2005", "", "Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan", "J.Phys.Soc.Jpn, 74(2005)412", "A.Tajima,A.Nakao,R.Kato", "", "" ] }, { "id": "269", "line_start": 254, "line_end": 254, "sha256": "bb8d4035c1cd9a25f87968ecdbb072c80c49a1b3662b4f0f6deb26343b028135", "values": [ "269", "P066020508", "Me4As", "beta'-Me4As[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "4", "", "", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. SC for b-axis pressure (7 < P < 10 kbar). not SC for a- and c-axis pressure.", "", "", "Uniaxial strain effect in a strongly correlated two-dimensional system beta'-(CH3)4As[Pd(dmit)2]2", "2002", "", "Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan", "Phys.Rev.B, 66(2002)020508R", "R.Kato,N.Tajima,M.Tamura,J.Yamaura", "", "" ] }, { "id": "270", "line_start": 255, "line_end": 255, "sha256": "9ab074f0144b1d79dac24ee87ba3a3d6a2a7822bfbf5b10c5ade7c1de806fc2d", "values": [ "270", "SSC1050561", "Me2Et2P", "beta'-Me2Et2P[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "4", "", "", "0.69", "", "", "", "-6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. Et=C2H5. SC-region: 6.9 =< P =< 10.4 kbar. Tc=1.8 K at P=10.4 kbar. R(H,T) measured at P=6.9 kbar. two dimensionality (r/B) = 0.82.", "", "", "A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)", "1998", "", "ISSP, The University of Tokyo,Tokyo,Japan", "Solid State Commun., 105(1998)561", "R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima", "", "" ] }, { "id": "271", "line_start": 256, "line_end": 256, "sha256": "c25477a08b59d5d70712beec02fdd93711a9c34ca288874fcd5111efde193a4b", "values": [ "271", "SSC1050561", "Me2Et2Sb", "beta'-Me2Et2Sb[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. Et=C2H5. not SC upto 10.4 kbar. two dimensionality (r/B) = 0.96.", "", "", "A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)", "1998", "", "ISSP, The University of Tokyo,Tokyo,Japan", "Solid State Commun., 105(1998)561", "R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima", "", "" ] }, { "id": "272", "line_start": 257, "line_end": 257, "sha256": "fd6bdd8a4c6798225d117f0c826efc716711f58877eb1d8bb484baf7adcb355a", "values": [ "272", "SYN1400151", "Hg2.9I8", "beta-(EDT-TTF)4Hg2.9I8", "", "EDT-TTF", "", "", "", "", "", "", "8.1", "", "", "0", "", "", "", "", "", "", "", "", "114", "", "", "", "", "", "", "", "", "OHC272", "", "", "", "", "COHERE(0) estimated from COHERE(1.43K)//=126A. nCOHERE(0)=22A from nCOHERE(1.43K)=25A. stoichiometry determined by EPMA.", "OHC272.dat", "", "New ambient pressure organic superconductor with Tc = 8.1 K based on unsymmetrical donor molecule, ethylenedithiotetrathiafulvalene: (EDT-TTF)4Hg3-zI8, z=0.1-0.2", "2004", "", "Institute of Problems of Chemical Physics, Russian Academy of Science, Chernogolovka 142432, MD, Russia", "Synth.Metals, 140(2004)151", "E.I.Zhilyaeva,S.A.Torunova,R.N.Lyubovskaya,G.A.Mousdis,G.C.Papavassiliou,J.A.A.J.Perenboom,S.I.Pesotskii,R.B.Lyubovskii", "", "" ] }, { "id": "273", "line_start": 258, "line_end": 258, "sha256": "c4b0cf85de8a6a2611be618171a51261fb820246c8efa97eb1d444eb802679d3", "values": [ "273", "CEM1590407", "FeCl4", "kappa-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "0.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.45", "", "", "", "", "", "AF comfirmed by SP-heat. AF easy axis = a-axis.", "", "", "Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions", "2001", "", "Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan", "J.Solid State Chem., 159(2001)407", "T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi", "", "" ] }, { "id": "274", "line_start": 259, "line_end": 259, "sha256": "6f215a1cb31f4b2c890a8931980e99665303041c4b4a9f516c548f36aed50943", "values": [ "274", "CEM1590407", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "2.5", "", "", "", "", "", "oriented crystal", "", "", "Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions", "2001", "", "Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan", "J.Solid State Chem., 159(2001)407", "T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi", "", "" ] }, { "id": "275", "line_start": 260, "line_end": 260, "sha256": "febb124458d8cbacb873f8c7891daef9b4da689a12aa32133f94de8fe1f044db", "values": [ "275", "CHL0870931", "Au(CN)2", "(DMET)2Au(CN)2", "", "DMET", "", "", "", "", "", "", "0.8", "", "", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at 25K.", "", "", "New organic superconductor, (DMET)2Au(CN)2", "1987", "", "", "Chem.Lett., (1987)931", "K.Kikuchi,M.Kikuchi,T.Namiki,K.Saito,I.Ikemoto,K.Murata,T.Ishiguro,K.Kobayashi", "", "" ] }, { "id": "276", "line_start": 261, "line_end": 261, "sha256": "d571a56b7076fc5371d6377d1c487dc756e6f2b856e0d5954f92b3112e97570e", "values": [ "276", "JMC0100245", "GaBr4", "kappa-(BETS)2GaBr4", "", "BETS", "", "", "", "", "", "", "1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc=0.5 - 1.0 K. Tc(on) = 1.3 K. Space-G = Pnma", "", "", "A new kappa-type organic superconductor based on BETS molecules, kappa- (BETS)2GaBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene]", "2000", "", "Institute for Molecular Science, Myodaiji-cho, Okazaki 444-8585, Japan", "J.Mater.Chem., 10(2000)245", "H.Tanaka,E.Ojima,H.Fujiwara,Y.Nakazawa,H.Kobayashi,A.Kobayashi", "", "" ] }, { "id": "277", "line_start": 262, "line_end": 262, "sha256": "42a7f4e4ce52638c6b8313510940d36801176afeaa052cd3594faec15f0d33c6", "values": [ "277", "JMC0112095", "[(H3O)Fe(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhNO2", "", "BEDT-TTF", "10.2732", "19.9494", "35.0304", "", "92.969", "", "6.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-0.16", "", "", "", "", "", "", "space-G = C2/c. Curie-C = 3.877 emu/mole. Structure parameters are at 120 K.", "", "", "New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)", "2001", "", "Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK", "J.Mater.Chem., 11(2001)2095", "S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs", "", "" ] }, { "id": "278", "line_start": 263, "line_end": 263, "sha256": "7012968b5ead77a787375209cb73644848933f41ea88d812c19e4bdc5484e4df", "values": [ "278", "JMC0112095", "[(NH4)Fe(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(NH4)Fe(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "6.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)", "2001", "", "Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK", "J.Mater.Chem., 11(2001)2095", "S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs", "", "" ] }, { "id": "279", "line_start": 264, "line_end": 264, "sha256": "54d77e48bdc4f30c5ab1ded6b88d22b5b832256a1b748a7391dbe25a0e381015", "values": [ "279", "JMC0112095", "[(H3O)Cr(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Cr(C2O4)3]:PhNO2", "", "BEDT-TTF", "10.2834", "19.9172", "34.939", "", "93.299", "", "5.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-1.44", "", "", "", "", "", "", "space-G = C2/c. Curie-C = 2.129 emu/mole. Tc (0) = 3.2 K. Structure parameters are at 120 K", "", "", "New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)", "2001", "", "Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK", "J.Mater.Chem., 11(2001)2095", "S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs", "", "" ] }, { "id": "280", "line_start": 265, "line_end": 265, "sha256": "847f0058bcead123dad048bd5dbc720d44c16f2bde3ec82a02e9a3d9a77a3728", "values": [ "280", "JMC0112095", "[(NH4)Cr(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(NH4)Cr(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "5.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)", "2001", "", "Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK", "J.Mater.Chem., 11(2001)2095", "S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs", "", "" ] }, { "id": "281", "line_start": 266, "line_end": 266, "sha256": "a7fe35ab228b6313211ad88531af29dc0b2309612ae423354e19ca44b568442b", "values": [ "281", "JMC0112410", "TlCl4", "kappa-(BETS)2TlCl4", "", "BETS", "", "", "", "", "", "", "2.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Space-G = Pnma. Slow cooling leads to destruction of crystals at about 220 K. Fast cool and annealing(170K) sample shows SC.", "", "", "A new molecular superconductor, kappa-(BETS)2TlCl4 [BETS = bis(ethylenedithio)tetraselenafulvalene]", "2001", "", "Institute for Molecular Science, Myodaiji, Okazaki 444, Japan", "J.Mater.Chem., 11(2001)2410", "V.Gritsenko,H.Tanaka,H.Kobayashi,A.Kobayashi", "", "" ] }, { "id": "282", "line_start": 267, "line_end": 267, "sha256": "0347fd4a11c6c1e38b61070f29b790969fba3c62854742df1e39da51a4793557", "values": [ "282", "SYN1021703", "Cu[N(CN)2]Br", "kappa-(ESET-TTF)2Cu[N(CN)2]Br", "", "ESET-TTF", "13.106", "30.244", "8.632", "", "", "", "4.7", "", "", "0.32", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC phase appears for very narrow pressure region; 3.2 =< SC < 3.5 kbar. Space-G = Pnma.", "", "", "A new synthesis of Se-containing TTF derivatives", "1999", "", "", "Synth.Met., 102(1999)1703", "Y.Okamoto,M.Iso,Y.Kashimura,J.Yamaura,R.Kato", "", "" ] }, { "id": "283", "line_start": 268, "line_end": 268, "sha256": "c4eea70b5cf4e03b8189c353f72ea3e2c01108e0f4e8fbf055cc984aea042fb7", "values": [ "283", "SYN1371239", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "10.3547", "20.1508", "35.542", "", "92.571", "", "7.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Space-G = C2/c. SC volume fraction = 31% at 1.8 K.", "", "", "Structures and properties of new superconductors, beta''-(ET)4[(H3O)Ga(C2O4)3]Sol [Sol = nitrobenzene and pyridine]", "2003", "", "", "Synth.Met., 137(2003)1239", "H.Akutsu,A.Akutsu-Sato,S.S.Turner,P.Day,D.A.Tocher,M.R.Probert,J.A.K.Howard,D.Le Pevelen,A.-K.Klehe,J.Singleton,V.N.Laukhin", "", "" ] }, { "id": "284", "line_start": 269, "line_end": 269, "sha256": "4f27b2c6b99a81db7ae6ca9847052bfb583c221855d70fb35ab823f67467568a", "values": [ "284", "SYN1371239", "[(H3O)Ga(C2O4)3]:pyridine", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:pyridine", "", "BEDT-TTF", "10.3605", "19.965", "35.428", "", "92.76", "", "1.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Space-G = C2/c", "", "", "Structures and properties of new superconductors, beta''-(ET)4[(H3O)Ga(C2O4)3]Sol [Sol = nitrobenzene and pyridine]", "2003", "", "", "Synth.Met., 137(2003)1239", "H.Akutsu,A.Akutsu-Sato,S.S.Turner,P.Day,D.A.Tocher,M.R.Probert,J.A.K.Howard,D.Le Pevelen,A.-K.Klehe,J.Singleton,V.N.Laukhin", "", "" ] }, { "id": "285", "line_start": 270, "line_end": 270, "sha256": "8cede9a3edcd6418617aa988f4de3a9df8a9a27fdafb9760eed480839ea4f9d2", "values": [ "285", "SYN1540245", "[(H3O)Cr(C2O4)3]:PhBr", "(BEDT-TTF)4[(H3O)Cr(C2O4)3]:PhBr", "", "BEDT-TTF", "10.287", "19.9773", "35.475", "90", "93.448", "90", "1.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "-0.12", "", "", "", "", "", "", "Space-G = C2/c. R is not zero at 0.4 K. Curie-C = 1.816 emu.K/mol.", "", "", "New magnetic conductors and superconductors on BEDT-TTF and BEDS-TTF", "2005", "", "Instituto de Ciencia Molecular, Unversidad de Valencia, Dr.Moliner 50, 46100 Burjasot, Spain", "Synth.Met., 154(2005)245", "E.Coronado,S.Curreli,C.Gimenez-Saiz,C.J.Gomez-Garcia", "", "" ] }, { "id": "286", "line_start": 271, "line_end": 271, "sha256": "b77157d0b07af8c2193fc3b56a7fe5d9da0fbe000182022e45fe8010454878a8", "values": [ "286", "SYN1540245", "[(H3O)Fe(C2O4)3]:PhBr", "(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhBr", "", "BEDT-TTF", "10.2875", "20.0546", "35.513", "90", "93.238", "90", "4", "", "", "0", "", "", "", "", "", "10", "8", "", "", "", "", "", "", "", "", "-0.05", "", "", "", "", "", "", "Space-G = C2/c. R is not zero at 0.4 K. Curie-C = 4.167 emu.K/mol. Hc2//b = 0.5 T, Hc2//c = 8 T.", "", "", "New magnetic conductors and superconductors on BEDT-TTF and BEDS-TTF", "2005", "", "Instituto de Ciencia Molecular, Unversidad de Valencia, Dr.Moliner 50, 46100 Burjasot, Spain", "Synth.Met., 154(2005)245", "E.Coronado,S.Curreli,C.Gimenez-Saiz,C.J.Gomez-Garcia", "", "" ] }, { "id": "287", "line_start": 272, "line_end": 272, "sha256": "f92d3ed5d0c19195e417900e30bfa5e2f4ff6ebd88d73ee41ca1e53e23b8e466", "values": [ "287", "CEM1680582", "Br", "kappa-(MDSe-TSF)2Br", "", "MDSe-TSF", "23.954", "11.1716", "8.9576", "", "99.298", "", "4", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G=C2/c, Chemical formula=C14H8Se12Br, formula weight = 1203.64. SC-volume = 0.5 - 4.0 %.", "", "", "Novel Conductive Radical Cation Salts Based on Methylenediselenotetraselenafulvalene (MDSe-TSF): A Sign of Superconductivity in kappa-(MDSe-TSF)2Br Below 4 K", "2002", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "J.Solid State Chem., 168(2002)582", "M.Kodani,A.Takamori,K.Takimiya,Y.Aso,T.Otsubo", "", "" ] }, { "id": "288", "line_start": 273, "line_end": 273, "sha256": "8eab5df501b3c91bbd474c13f9d1058557d527fc409b84d3b52d6aeb4a1cd9d9", "values": [ "288", "CHL0871819", "Me4N", "Me4N[Ni(dmit)2]2", "", "Ni(dmit)2", "13.675", "6.476", "36.048", "", "94.74", "", "5", "5", "0.7", "0.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me = CH3. (dTc/dP) at Pcrit is positive. Thermal expansion coeff. = 7.7(//a), 3.2(//b), 2.5 (c//) in unit of E-5 /K.", "", "", "The first molecular superconductor based on pai-acceptor molecules and closed-shell cations, [(Ch3)4N][Ni(dmit)2]2, low-temperature X-ray studies and superconducting transition", "1987", "", "Department of Chemistry,Faculty of Science, The University of Tokyo,Tokyo, Japan", "Chem.Lett., 1987, 1819-1822", "A.Kobayashi,H.Kim,Y.Sasaki,R.Kato,H.Kobayashi,S.Moriyama,Y.Nishio,K.Kajita,W.Sasaki", "", "" ] }, { "id": "289", "line_start": 274, "line_end": 274, "sha256": "1d6d55d621ed25bf46bc0896a56328192364354b0f46930c9775b463e93ed028", "values": [ "289", "CHL0931235", "Ni(dmit)2", "alpha-(EDT-TTF)[Ni(dmit)2]", "", "EDT-TTF", "", "", "", "", "", "", "1.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "First ambient-pressure superconductor based on Ni(dmit)2, alpha-EDT-TTF[Ni(dmit)2]", "1993", "", "Department of Chemistry,Faculty of Science, The University of Tokyo,Tokyo, Japan", "Chem.Lett., 1993, 1235-1238", "H.Tajima,M.Inokuchi,A.Kobayashi,T.Ohta,R.Kato,H.Kobayashi,H.Kuroda", "", "" ] }, { "id": "290", "line_start": 275, "line_end": 275, "sha256": "5ba21568eadc1b6df9b77166a55540a41a12da0d94b6fce6d4d22e71ede313e5", "values": [ "290", "CHL0912163", "Me4N", "beta-Me4N[Pd(dmit)2]2", "", "Ni(dmit)2", "14.523", "6.32", "35.134", "", "90.94", "", "6.2", "6.2", "0.65", "0.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me = CH3. space-G = C2/c. Tc = Tc(mid).", "", "", "New molecular superconductor, beta-[(CH3)4N][Pd(dmit)2]2", "1991", "", "Department of Chemistry,Faculty of Science, The University of Tokyo,Tokyo, Japan", "Chem.Lett., 1991, 2163-2166", "A.Kobayashi,H.Kobayashi,A.Miyamoto,R.Kato,R.A.Clark,A.E.Underhill", "", "" ] }, { "id": "291", "line_start": 276, "line_end": 276, "sha256": "93a1bfe18b8d7a0033ee019b81eab7de9e4455809f916777565a9c36cfc6dba3", "values": [ "291", "CHM0151225", "I3", "beta-(MDT-ST)I1.27", "", "MDT-ST", "", "", "", "", "", "", "3.6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(SUS) = 3.8 K.", "", "", "Organic Superconductors Based on a New Electron Donor, Methylenedithio-diselenadithiafulvalene (MDT-ST)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)1225", "K.Takimiya,A.Takamori,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "292", "line_start": 277, "line_end": 277, "sha256": "8d6c56540069d503da5cf7c351566d22e625fba2c3a8ea66a81838a2b2f2c472", "values": [ "292", "CHM0151225", "I2Br", "beta-(MDT-ST)I1.07Br0.2", "", "MDT-ST", "", "", "", "", "", "", "3.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(SUS) = 3.8 K.", "", "", "Organic Superconductors Based on a New Electron Donor, Methylenedithio-diselenadithiafulvalene (MDT-ST)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)1225", "K.Takimiya,A.Takamori,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "293", "line_start": 278, "line_end": 278, "sha256": "af11d98f7dd63267f6efca50f999f745b5ebf493b4cb6f2473fe6cb9d2a8f04f", "values": [ "293", "CHM0153250", "I3", "beta-(MDT-TSF)I1.27", "", "MDT-TSF", "4.013", "12.539", "25.62", "", "", "", "4.6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "orthorhombic, space-G = Pnma. Chemical formula = C7H4S2Se4I1.27. Tc(SUS) = 4.4 K. SC-volume = 90 %.", "", "", "New Organic Superconductors with an Incommensurate Anion Lattice Consisting of Polyhalide Chains (MDT-TSF)Xy (MDT-TSF ) = Methylenedithiotetraselenafulvalene; X = Halogen; y = 1.27-1.29)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)3250", "K.Takimiya,M.Kodani,Y.Kataoka,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "294", "line_start": 279, "line_end": 279, "sha256": "ae1bc5d9f0c9f26f4a999a99161d65af31b458dc6614c9ea02d1f930ce8b1479", "values": [ "294", "CHM0153250", "I2Br", "beta-(MDT-TSF)I1.19Br0.08", "", "MDT-TSF", "4.01", "12.543", "25.584", "", "", "", "5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "orthorhombic, space-G = Pnma. Chemical formula = C7H4S2Se4I1.19Br0.08. Tc(SUS) = 4.8 K. SC-volume = 100 %.", "", "", "New Organic Superconductors with an Incommensurate Anion Lattice Consisting of Polyhalide Chains (MDT-TSF)Xy (MDT-TSF ) = Methylenedithiotetraselenafulvalene; X = Halogen; y = 1.27-1.29)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)3250", "K.Takimiya,M.Kodani,Y.Kataoka,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "295", "line_start": 280, "line_end": 280, "sha256": "bb961afdbf4cd92563599a7437de4e516815908c7fbd4815c3d81d4a7e08260d", "values": [ "295", "CHM0153250", "I2Br", "beta-(MDT-TSF)I0.77Br0.52", "", "MDT-TSF", "4.026", "12.515", "25.315", "", "", "", "4", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "orthorhombic, space-G = Pnma. Chemical formula = C7H4S2Se4I0.77Br0.52. Tc(SUS) = 4.0 K. SC-volume = 40 %.", "", "", "New Organic Superconductors with an Incommensurate Anion Lattice Consisting of Polyhalide Chains (MDT-TSF)Xy (MDT-TSF ) = Methylenedithiotetraselenafulvalene; X = Halogen; y = 1.27-1.29)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)3250", "K.Takimiya,M.Kodani,Y.Kataoka,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "296", "line_start": 281, "line_end": 281, "sha256": "5c43642c8ecbe5e7645d3c4aab6630f31675e80b40f8ca2c9f979ddcdd468abd", "values": [ "296", "CHM0153250", "I3", "beta-(MDT-TSF)I1.27", "", "MDT-TSF", "4.012", "12.546", "25.635", "", "", "", "5.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Anion = I1.27-zClz (z nearly zero). orthorhombic, space-G = Pnma. Chemical formula = C7H4S2Se4I1.27. Tc(SUS) = 5.0 K. SC-volume = 100 %.", "", "", "New Organic Superconductors with an Incommensurate Anion Lattice Consisting of Polyhalide Chains (MDT-TSF)Xy (MDT-TSF ) = Methylenedithiotetraselenafulvalene; X = Halogen; y = 1.27-1.29)", "2003", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 15(2003)3250", "K.Takimiya,M.Kodani,Y.Kataoka,Y.Aso,T.Otsubo,T.Kawamoto,T.Mori", "", "" ] }, { "id": "297", "line_start": 282, "line_end": 282, "sha256": "4e6888ce1afb83e177f87364d52b9035052cf588563ee423089ade20a225fcc3", "values": [ "297", "CHM0165120", "AuI2", "beta-(MDT-TS)(AuI2)0.441", "", "MDT-TS", "3.994", "12.448", "25.119", "", "", "", "4.7", "", "", "1.14", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "orthorhombic, space-G = Pnma, Chemical formula = C7H4S4Se2Au0.441I0.882. T = 50 K. R(H,T) measured for H < 5 T at 11.4 kbar.", "", "", "Pressure-Induced Superconductivity in (MDT-TS)(AuI2)0.441 [MDT- TS ) = 5H-2-(1,3-diselenol-2-ylidene)-1,3,4,6-tetrathiapentalene]: A New Organic Superconductor Possessing an Incommensurate Anion Lattice", "2004", "", "Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, 739-8527, Japan", "Chem.Mater., 16(2004)5120", "K.Takimiya,M.Kodani,N.Niihara,Y.Aso,T.Otsubo,Y.Bando,T.Kawamoto,T.Mori", "", "" ] }, { "id": "298", "line_start": 283, "line_end": 283, "sha256": "c3e303c51fa66e120634be4096816a4a953fa8b3714962ed9149f27aa3b92530", "values": [ "298", "SSC0650361", "Me4N", "Me4N[Ni(dmit)2]2", "", "Ni(dmit)2", "", "", "", "", "", "", "3", "", "", "0.32", "", "", "", "", "", "", "", "", "290", "", "", "", "", "", "", "", "", "", "", "", "", "", "hydrostatic pressure upto 15 kbar. Tc(7kbar) = 5.0 K. Hc2(defined as R=0.5R0) is linearfunction ob T.", "", "", "Transport properties of ((CH3)4N)(Ni(dmit)2)2: A new organic superconductor", "1988", "", "", "Solid State Commun., 65(1988)361", "K.Kajita,Y.Nishio,S.Moriyama,R.Kato,H.Kobayashi,W.Sasaki,A.Kobayashi,H.Kim,Y.Sasaki", "", "" ] }, { "id": "299", "line_start": 284, "line_end": 284, "sha256": "4019be9a790fdecf33c420037b11a86ad8b6ca05574e1efcc91aa940ac6516d4", "values": [ "299", "SSC1080377", "Cu[N(CN)2]Br", "kappa-(BEDSe-TTF)2Cu[N(CN)2]Br", "", "BEDSe-TTF", "13.23", "30.39", "8.694", "", "", "", "7.5", "", "", "0.15", "", "", "", "-35", "", "", "", "", "", "", "", "", "", "", "", "-0.2", "", "", "", "", "", "", "Space-G = Pnma. T = 50 K at ambient-P. Tc decreases with P, goes to zero at P=0.3 GPa.", "", "", "Superconductivity in new organic conductor kappa-(BEDSe-TTF)2CuN(CN)2Br", "1998", "", "", "Solid State Commun., 108(1998)377", "J.Sakata,H.Sato,A.Miyazaki,T.Enoki,Y.Okano,R.Kato", "", "" ] }, { "id": "300", "line_start": 285, "line_end": 285, "sha256": "7b8672a06c4ce6d118393e6afe0740e3bcd2770b1e9f6fd35e190c95f17c40d8", "values": [ "300", "SYN0610199", "AuI2", "(DMET-TSeF)2AuI2", "", "DMET-TSeF", "7.799", "15.869", "6.74", "98.16", "104.49", "89.48", "0.58", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "301", "line_start": 286, "line_end": 286, "sha256": "736879c009970b8362056c737417afcdd965ba354081204a168c12c7fe32e415", "values": [ "301", "SYN0700861", "I3", "(DMET-TSeF)2I3", "", "DMET-TSeF", "", "", "", "", "", "", "0.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Superconductivity and field induced states in DMET-TSeF family", "1995", "", "", "Synth.Met., 70(1995)861", "K.Oshima,H.Okuno,K.Kato,R.Maruyama,R.Kato,A.Kobayashi,H.Kobayashi", "", "" ] }, { "id": "302", "line_start": 287, "line_end": 287, "sha256": "8126f7aa614535ee4ec91501fac76b183a183ce6b6e0b692eb0fe40eb5a5aad5", "values": [ "302", "ADV0040033", "ClO4", "kappa-((s,s)-DMBEDT-TTF)2ClO4", "", "DMBEDT-TTF", "", "", "", "", "", "", "2.6", "", "", "0.58", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc decreases with P. Tc(10kbar) = 0 K.", "", "", "Crystal structure and electrical properties of kappa-((s,s)-(DMBEDT-TTF)2ClO4", "1992", "", "", "Adv.Mater., 4(1992)33", "J.S.Zambounis,C.W.Mayer,K.Hauenstein,B.Hilti,W.Hofherr,J.Pfeiffer,M.Burkle,G.Rihs", "", "" ] }, { "id": "303", "line_start": 288, "line_end": 288, "sha256": "5472d466e984aa182f6d0d11960c75e8be779a18acc1d2e51090ce4410cc3ed9", "values": [ "303", "JTL0410081", "I3", "beta-(BEDT-TTF)2I3", "", "BEDT-TTF", "", "", "", "", "", "", "1.5", "7.5", "0.12", "0", "", "", "", "-20", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Effect of pressure on the superconductivity of beta-(BEDT-TTF)2I3", "1985", "", "", "JETP Lett., 41(1985)81", "V.N.Laukhin,E.E.Kostyuchenko,Yu.V.Sushko,I.F.Shchegolev,E.B.Yagubskii", "", "" ] }, { "id": "304", "line_start": 289, "line_end": 289, "sha256": "35fc2a7adfb1ad45803bb5a041a22db4aa78cbb7735fb7e8862ef92280cb19ab", "values": [ "304", "JTL0401201", "I3", "alpha-(BEDT-TTF)2I3", "", "BEDT-TTF", "10.785", "9.172", "17.39", "82.08", "96.92", "89.13", "3.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "I-doped crystal prepared by holding in the saturated I-vapor for 1h at 25C. 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"", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(mid) = 4.29 K. dTc(10-90%) = 1.47 K.", "", "", "New organic superconductors in the system (ET)2M(CF3)4(solvent) (M=Cu,Ag,Au): Dramatic effects of organometallic anion and solvent replacement", "1996", "", "", "Mol.Cryst.Liq.Cryst., 285(1996)43", "J.A.Schlueter,J.M.Williams,Urs Geiser,H.H.Wang,A.M.Kini,M.E.Kelly,J.D.Dudek", "", "" ] }, { "id": "321", "line_start": 306, "line_end": 306, "sha256": "53251cb3b0baf8846f89d2410c9335f4e88937b70b0e12490c649d6d9bab1f0d", "values": [ "321", "MOL2850043", "Ag(CF3)4(TBE)", "kappa-(h8-BEDT-TTF)2Ag(CF3)4(TBE)", "", "BEDT-TTF", "", "", "", "", "", "", "4.84", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(mid) = 3.92 K. dTc(10-90%) = 1.39 K.", "", "", "New organic superconductors in the system (ET)2M(CF3)4(solvent) (M=Cu,Ag,Au): Dramatic effects of organometallic anion and solvent replacement", "1996", "", "", "Mol.Cryst.Liq.Cryst., 285(1996)43", "J.A.Schlueter,J.M.Williams,Urs Geiser,H.H.Wang,A.M.Kini,M.E.Kelly,J.D.Dudek", "", "" ] }, { "id": "322", "line_start": 307, "line_end": 307, "sha256": "282b5c44113e00a71308cc99f22ae3091074ba223e4cc504704b0089c5b30a36", "values": [ "322", "MOL2840195", "Ag(CF3)4(TCE)", "kappa-(BEDT-TTF)2Ag(CF3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "11.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "323", "line_start": 308, "line_end": 308, "sha256": "aba1f935a3af3c7e234e1b8db3b12cf4d973909629fdf3a86433cbf4f9fbca2c", "values": [ "323", "MOL2840195", "Au(CF3)4(TCE)", "kappa-(BEDT-TTF)2Au(CF3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "10.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "324", "line_start": 309, "line_end": 309, "sha256": "de02cbfee601eb7d83ed57940f3e214dc4a58af737a208f8aa81b8dfeccee444", "values": [ "324", "MOL2840195", "Cu(CF3)4(TCE)", "kappa-(BEDT-TTF)2Cu(CF3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "9.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "325", "line_start": 310, "line_end": 310, "sha256": "580203bb069cfc7168e2a647109805b4f3c4590d0888421ee9853397e32028d9", "values": [ "325", "MOL2840195", "Ag(CF3)4(BDCE)", "kappa-(BEDT-TTF)2Ag(CF3)4(211BDCE)", "", "BEDT-TTF", "", "", "", "", "", "", "10.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "326", "line_start": 311, "line_end": 311, "sha256": "255bb65b36127fbc7c2e0c2bc3c808737804f9ee084d91927c0ce459e8ef552f", "values": [ "326", "MOL2840195", "Ag(CF3)4(BDCE)", "kappa-(BEDT-TTF)2Ag(CF3)4(112BDCE)", "", "BEDT-TTF", "", "", "", "", "", "", "7.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "327", "line_start": 312, "line_end": 312, "sha256": "128b45b01c659afff788a3e6b5073e34fb8d90365df360d72b898e70eadba0a8", "values": [ "327", "MOL2840195", "Ag(CF3)4(TBE)", "kappa-(BEDT-TTF)2Ag(CF3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "7.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "kappa phase is needle-like crystal. Tc determined by ac-SUS.", "", "", "Synthesis and physical properties of a novel, highly tunable family of organic superconductors: (ET)2M(CF3)4(1,1,2-trihaloethane) (M=Cu,Ag,Au)", "1996", "", "", "Mol.Cryst.Liq.Cryst., 284(1996)195", "J.A.Schlueter,Urs Geiser,H.H.Wang,M.E.Kelly,J.D.Dudek,J.M.Williams,D.Naumann,T.Roy", "", "" ] }, { "id": "328", "line_start": 313, "line_end": 313, "sha256": "84e88c9e04f5f0a93f9267c56210076ce1989e8493cbfeef4663249290fe8036", "values": [ "328", "JTL0420468", "Hg3Cl8", "(BEDT-TTF)4Hg3Cl8", "", "BEDT-TTF", "11.062", "8.754", "35.92", "", "91.01", "", "1.8", "", "", "1.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G = I2/c", "", "", "Superconductivity in a BEDT-TTF organic conductor with a chloromercurate anion", "1985", "", "", "JETP Lett., 42(1985)468", "R.N.Lyubovskaya,R.B.Lyubovskii,R.P.Shibaeva,M.Z.Aldoshina,L.M.Gol'denberg,L.P.Rozenberg,M.L.Khidekel',Yu.F.Shul'pyakov", "", "" ] }, { "id": "329", "line_start": 314, "line_end": 314, "sha256": "d2053573d3aebefad14e05317b91eb5c1d58c45d11d6d0652fe042607f4f3992", "values": [ "329", "PRL0783555", "PF6", "(TMTSF)2PF6", "3", "TMTSF", "", "", "", "", "", "", "1.13", "", "", "0.6", "", "", "", "", "", "", "6", "", "", "", "", "", "", "", "", "", "", "OHC329", "", "", "", "", "Hc2(0) shows Hc2(0.11K)//b-axis. Hc2//a, //b, //c-axis were measured. Figure shows Hc2(T) at P = 0.6 GPa.", "OHC329.dat", "", "Anisotropy of the Upper Critical Field in (TMTSF)2PF6", "1997", "", "Departments of Physics and Chemistry, State University of New York, Buffalo, New York 14260", "Phys.Rev.Lett., 78(1997)3555", "I.J.Lee,M.J.Naughton,G.M.Danner,P.M.Chaikin", "", "" ] }, { "id": "330", "line_start": 315, "line_end": 315, "sha256": "199b855f76d6e83676d2679e55255c38f69a82a8a33ce35eb195b11cba9c1bc6", "values": [ "330", "PR06214670", "PF6", "(TMTSF)2PF6", "3", "TMTSF", "", "", "", "", "", "", "1.18", "", "", "0.57", "", "", "", "", "", "", "10", "", "", "", "", "", "", "", "", "", "", "OHC330", "OPH330", "", "", "", "Hc2(T) at P = 5.7 kbar and phase diagram for H//b-axis.", "OHC330.dat", "OPH330.dat", "Exceeding the Pauli paramagnetic limit in the critical field of (TMTSF)2PF6", "2000", "", "Department of Physics, Princeton University, Princeton, New Jersey 08544", "Phys.Rev.B, 62(2000)R14669", "I.J.Lee,P.M.Chaikin,M.J.Naughton", "", "" ] }, { "id": "331", "line_start": 316, "line_end": 316, "sha256": "4ee80d9753d433d20458168f4a01c7ac7f427e015a37be5e11612d2ec0e1cc9e", "values": [ "331", "ACS1223238", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "1.4", "1.8", "5.4", "5.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH331", "", "", "", "", "Prepared from acetonitrile solution with TMTTF, [Bu4N][PF6]", "OPH331.dat", "", "Superconducting transition of (TMTTF)2PF6 above 50 kbar [TMTTF = Tetramethyltetrathiafulvalene]", "2000", "", "Institute for Molecular Science,Okazaki 444-8585,Japan", "J.Am.Chem.Soc., 122(2000)3238", "T.Adachi,E.Ojima,K.Kato,H.Kobayashi,T.Miyazaki,M.Tokumoto,A.Kobayashi", "", "" ] }, { "id": "332", "line_start": 317, "line_end": 317, "sha256": "bf3eafc3c09a887b5e4c641098b1cab1b60cc79c9934e7f0866887ed9b89d8bb", "values": [ "332", "P074104504", "Cu[N(CN)2]Cl", "kappa'-(BEDT-TTF)2Cu[N(CN)2]Cl", "3", "BEDT-TTF", "12.929", "29.879", "8.457", "", "", "", "11.9", "", "", "0", "", "", "", "", "", "", "", "1.36", "", "", "", "", "", "", "", "", "", "OHC332", "", "", "", "", "ambient pressure SC. (dHc2/dT)//b = 0.075 T/K. (dHc2/dT)//ac = 1.36 T/K. lattice const. at 297 K.", "OHC332.dat", "", "Transport properties and structural features of the ambient-pressure superconductor kappa'-(BEDT-TTF)2Cu[N(CN)2]Cl", "2006", "", "Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka, Moscow Region, 142432 Russia", "Phys.Rev.B, 74(2006)104504", "V.N.Zverev,A.I.Manakov,S.S.Khasanov,R.P.Shibaeva,N.D.Kushch,A.V.Kazakova,L.I.Buravov,E.B.Yagubski,E.Canadell", "", "" ] }, { "id": "333", "line_start": 318, "line_end": 318, "sha256": "de3803187e532117dd6e88d7294de35cc9440daec03b60a35514941e56ba0f48", "values": [ "333", "P074104504", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "3", "BEDT-TTF", "12.963", "29.897", "8.467", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "lattice const. at 293 K.", "", "", "Transport properties and structural features of the ambient-pressure superconductor kappa'-(BEDT-TTF)2Cu[N(CN)2]Cl", "2006", "", "Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka, Moscow Region, 142432 Russia", "Phys.Rev.B, 74(2006)104504", "V.N.Zverev,A.I.Manakov,S.S.Khasanov,R.P.Shibaeva,N.D.Kushch,A.V.Kazakova,L.I.Buravov,E.B.Yagubski,E.Canadell", "", "" ] }, { "id": "334", "line_start": 319, "line_end": 319, "sha256": "9c4c54054294e08ed1d04af190fbce2705d0b1131604c12fc7578a6930bb4d02", "values": [ "334", "SSC1370637", "CsCd(SCN)4", "alpha-(BEDT-TTF)2CsCd(SCN)4", "3", "BEDT-TTF", "10.198", "20.35", "9.95", "92.63", "90.27", "88.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC(T > 0.6, P < 5 kbar). tricrinic. R measured for 0.6 < T < 300K. metallic behavior.", "", "", "Structural and electronic properties of a new molecular conductor, alpha-(BEDT-TTF)2CsCd(SCN)4", "2006", "", "Department of Basic Science, University of Tokyo, 3-8-1, Komaba, Meguro-ku, Tokyo 153-8902, Japan", "Solid State Commun., 137(2006)637", "R.Kondo,M.Higa,S.Kagoshima", "", "" ] }, { "id": "335", "line_start": 320, "line_end": 320, "sha256": "9fed4938b20ee8615486c3834d6cc6bb192fd6c2b469a1e802a5f2fb5ffe2126", "values": [ "335", "JJP0452264", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "7.9", "", "", "", "", "", "", "", "", "", "", "tunneling by STM. gap(d) = 2.1 - 3.9 meV. (2d/kTc) = 4.3 - 7.9.", "", "", "Scanning Tunneling Spectroscopy on Organic Superconductors", "2006", "", "Division of Physics, Hokkaido University, Sapporo 060-0810, Japan", "Jpn J.Appl.Phys.B, 45(2006)2264", "K.Ichimura,K.Nomura,A.Kawamoto", "", "" ] }, { "id": "336", "line_start": 321, "line_end": 321, "sha256": "ec06a41570cccaa245c60ee125bb226845f98d50635c927db052d5478b4451f0", "values": [ "336", "JJP0452264", "Cu[N(CN)2]Br", "kappa-(d[2:2]-BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "12", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "9.3", "", "", "", "", "", "", "", "", "", "", "partially deutrated salt. tunneling by STM. gap(d) = 3.0 - 4.8 meV. (2d/kTc) = 5.8 - 9.3.", "", "", "Scanning Tunneling Spectroscopy on Organic Superconductors", "2006", "", "Division of Physics, Hokkaido University, Sapporo 060-0810, Japan", "Jpn J.Appl.Phys.B, 45(2006)2264", "K.Ichimura,K.Nomura,A.Kawamoto", "", "" ] }, { "id": "337", "line_start": 322, "line_end": 322, "sha256": "5b40a4cd09f7c3407c9c0c67198cee4544e1e2593678e5643298d7d874c1918f", "values": [ "337", "JJP0452264", "Cu[N(CN)2]Br", "kappa-(d[3:3]-BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "12.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "6.4", "", "", "", "", "", "", "", "", "", "", "partially deutrated salt. tunneling by STM. gap(d) = 1.4 - 3.3 meV. (2d/kTc) = 2.7 - 6.4.", "", "", "Scanning Tunneling Spectroscopy on Organic Superconductors", "2006", "", "Division of Physics, Hokkaido University, Sapporo 060-0810, Japan", "Jpn J.Appl.Phys.B, 45(2006)2264", "K.Ichimura,K.Nomura,A.Kawamoto", "", "" ] }, { "id": "338", "line_start": 323, "line_end": 323, "sha256": "b35ba0064d5d5175ca10d88fb0f0ea824b4f7851b366a7f0e5da3128c58b3566", "values": [ "338", "P071052501", "AuI2", "(MDT-TS)(AuI2)0.441", "", "MDT-TS", "", "", "", "", "", "", "3.2", "", "", "1.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC338", "", "", "", "", "Tc(on) = 4.3 K. T = 50 K. Figure shows pressure dependence of T, Tc(mid), Tc(on) .", "OTC338.dat", "", "Superconductivity competing with the incommensurate antiferromagnetic insulating state in the organic conductor (MDT-TS)(AuI2)0.441", "2005", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan", "Phys.Rev.B, 71(2005)052501", "T.Kawamoto,Y.Bando,T.Mori,K.Takimiya,T.Otsubo", "", "" ] }, { "id": "339", "line_start": 324, "line_end": 324, "sha256": "6ed1d082e12492d34f3d6b9b1ab2f4c5de428f675a20ff788d4eeabb63edd16e", "values": [ "339", "EPL0720645", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x", "", "TMTSF", "", "", "", "", "", "", "1.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC339", "", "", "", "", "Tc means Tc(on). Figure shows Tc,T vs residual resistivity(Ohm.cm).", "OTC339.dat", "", "Impurity-controlled superconductivity/spin density wave interplay in the organic superconductor: (TMTSF)2ClO4", "2005", "", "Laboratoire de Physique des Solides (UMR 8502) - Universite Paris-Sud 91405, Orsay, France", "Euroohys.Lett., 72(2005)645", "N.Joo,P.Auban-Senzier,C.R.Pasquier,D.Jerome,K.Bechgaad", "", "" ] }, { "id": "340", "line_start": 325, "line_end": 325, "sha256": "7d9a8c2082b447c713d799450ea7497e8172de7ad6a27d361a4e029556e3989c", "values": [ "340", "JTL0820093", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "3", "BEDT-TTF", "12.932", "29.877", "8.458", "", "", "", "11.5", "", "", "0", "", "", "", "", "", "", "", "1.36", "", "", "", "", "", "", "", "", "", "OHC340", "", "", "", "", "cond. plane = ac plane. anisotropy Rb/Rac = 200 - 400 (300K), 1000 - 1400 (15K). Hc2 measured by ab plane current. (dHc2/dT) data for H//ac.", "OHC340.dat", "", "Superconductivity at normal pressure in kappa-(BEDT-TTF)2Cu[N(CN)2]Cl crystals", "2005", "", "", "JETP Lett., 82(2005)93", "E.B.Yagubskii,N.D.Kushch,A.V.Kazakova,L.I.Buravov,V.N.Zverev,A.I.Manakov,S.S.Khasanov,R.P.Shibaeva", "", "" ] }, { "id": "341", "line_start": 326, "line_end": 326, "sha256": "091bfa1515f0c9403f956f5128df65910fd1e7271057198350648a9598fb2bed", "values": [ "341", "P074212508", "Cu2(CN)3", "kappa-(BEDT-TTF)2Cu2(CN)3", "3", "BEDT-TTF", "", "", "", "", "", "", "4.7", "", "", "0.35", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC disappears at P=0.8 GPa. Insulator-to metal transition at 0.3 GPa. <13>C NMR measured.", "", "", "Suppression of inhomogeneous electron localization in kappa-(BEDT-TTF)2Cu2(CN)3 under pressure", "2006", "", "Division of Physics, Graduate School of Science, Hokkaido University. Kita-ku, Sapporo, Hokkaido 060-0810, Japan", "Phys.Rev.B, 74(2006)212508", "A.Kawamoto,Y.Honma,K.Kumagai,N.Matsunaga,K.Nomura", "", "" ] }, { "id": "342", "line_start": 327, "line_end": 327, "sha256": "988094db5ff4d31138c18f475d574f5f03dfbdb6d1419f277fe17849766526f6", "values": [ "342", "JPS0651340", "Cu2(CN)3", "kappa'-(BEDT-TTF)2Cu2(CN)3", "3", "BEDT-TTF", "16.111", "8.56", "13.331", "", "112.94", "", "5.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC342", "", "", "", "", "Tc depends on Cu(2+) content, which seems to increase with the growth rate of crystals. The content of Cu(2+) determined by ESR.", "OTC342.dat", "", "Realization of superconductivity at ambient pressure by band-filling control in kappa-(BEDT-TTF)2Cu2(CN)3", "1996", "", "Department of Chemistry, Kyoto University, Japan", "J.Phys.Soc.Jpn, 65(1996)1340", "T.Komatsu,N.Matsukawa,T.Inoue,G.Saito", "", "" ] }, { "id": "343", "line_start": 328, "line_end": 328, "sha256": "dd7ddbea6172d563c1dbc7ff91f60e7045f7bee067e828576855a0c98617033d", "values": [ "343", "JPS0651340", "Cu2(CN)3", "kappa-(BEDT-TTF)2Cu2(CN)3", "", "BEDT-TTF", "", "", "", "", "", "", "3.9", "", "", "0.06", "", "", "", "-16", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTP343", "OTC343", "", "", "", "", "OTP343.dat", "OTC343.dat", "Realization of superconductivity at ambient pressure by band-filling control in kappa-(BEDT-TTF)2Cu2(CN)3", "1996", "", "Department of Chemistry, Kyoto University, Japan", "J.Phys.Soc.Jpn, 65(1996)1340", "T.Komatsu,N.Matsukawa,T.Inoue,G.Saito", "", "" ] }, { "id": "344", "line_start": 329, "line_end": 329, "sha256": "7ec71d7575293665b721ec253fc41ce5552b65cdaf5a02ee1edadc4bf80e0558", "values": [ "344", "JPS0651340", "Cu2(CN)3", "kappa-(d8-BEDT-TTF)2Cu2(CN)3", "", "BEDT-TTF", "", "", "", "", "", "", "4.4", "", "", "0.01", "", "", "", "-16", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "deutrated", "", "", "Realization of superconductivity at ambient pressure by band-filling control in kappa-(BEDT-TTF)2Cu2(CN)3", "1996", "", "Department of Chemistry, Kyoto University, Japan", "J.Phys.Soc.Jpn, 65(1996)1340", "T.Komatsu,N.Matsukawa,T.Inoue,G.Saito", "", "" ] }, { "id": "345", "line_start": 330, "line_end": 330, "sha256": "657c0161c3fad4248e0e045d0b166c12ddc1ebc4729beec7a170a87583fe99f5", "values": [ "345", "JPS0651340", "Cu2(CN)3", "kappa'-(BEDT-TTF)2Cu2(CN)3", "", "BEDT-TTF", "", "", "", "", "", "", "4.1", "", "", "0", "", "", "", "-13", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC345", "", "", "", "", "", "OTC345.dat", "", "Realization of superconductivity at ambient pressure by band-filling control in kappa-(BEDT-TTF)2Cu2(CN)3", "1996", "", "Department of Chemistry, Kyoto University, Japan", "J.Phys.Soc.Jpn, 65(1996)1340", "T.Komatsu,N.Matsukawa,T.Inoue,G.Saito", "", "" ] }, { "id": "346", "line_start": 331, "line_end": 331, "sha256": "06c2454555bb45ada90182f1ba05251dc855a10d293287b249169253456af1de", "values": [ "346", "JPS0651340", "Cu2(CN)3", "kappa'-(d8-BEDT-TTF)2Cu2(CN)3", "", "BEDT-TTF", "", "", "", "", "", "", "5.7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "deutrated", "", "", "Realization of superconductivity at ambient pressure by band-filling control in kappa-(BEDT-TTF)2Cu2(CN)3", "1996", "", "Department of Chemistry, Kyoto University, Japan", "J.Phys.Soc.Jpn, 65(1996)1340", "T.Komatsu,N.Matsukawa,T.Inoue,G.Saito", "", "" ] }, { "id": "347", "line_start": 332, "line_end": 332, "sha256": "4ab0f9ff07e417ead0f3597acfd844f9bc290c575ec678f181ad50beea7e78c6", "values": [ "347", "SSC0790057", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "22", "210", "", "", "", "", "", "", "", "SP-heat measured for H//b-axis. (dC/gamma*Tc) = 2 +- 0.5 mJ/mol.K2", "", "", "SPECIFIC HEAT OF THE HIGH TC ORGANIC SUPERCONDUCTOR K-(ET)2CU(N(CN)2)BR", "1991", "", "", "SOLID STATE COMMUN,79(1991)57", "B.ANDRAKA,C.S.JEE,G.R.STEWART,J.S.KIM", "", "" ] }, { "id": "348", "line_start": 333, "line_end": 333, "sha256": "5a4562a1016fb7a569771a636d80c52b13255d99316739e9cc2df42b9979d92a", "values": [ "348", "JMC0051659", "Cu[N(CN)2]Br", "kappa-(BETS)2Cu[N(CN)2]Br", "", "BETS", "12.961", "31.005", "8.576", "", "", "", "", "", "", "", "", "", "", "", "1.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC upto 5 kbar. electrochemical method. space-G = Pnma. XRD at 293 K. formula=C22H16N3S8Se8CuBr.", "", "", "20 K crystal structure, electrical transport, electronic band structure, scanning tunnelling microscopy and pressure-RF impedance studies on the organic conducting salt kappa-(BEDT-TSF)2Cu[N(CN)2]Br", "1995", "", "", "J.Mater.Chem., 5(1995)1659", "T.Burgin,T.Miebach,J.C.Huffman,L.K.Montgomery,J.A.Paradis,C.Rovira,M-H.Whangbo,S.N.Magonov,S.I.Khan,C.E.Strouse,D.L.Overmyer,J.E.Schirber", "", "" ] }, { "id": "349", "line_start": 334, "line_end": 334, "sha256": "b2c841a95b730e441b19c776afc4db15c2510d6b0b1e6760a6e27070655c2602", "values": [ "349", "JMC0120159", "[Au(CN)4]", "theta-(DIETS)2[Au(CN)4]", "", "DIETS", "4.274", "11.114", "37.426", "", "", "", "8.6", "", "", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC under uniaxial strain along c-axis (perpendicular to the donor layer). C20H8N4AuI4S8Se4 (M=1581.21, ortho, Pnnm)", "", "", "A supramolecular superconductor theta-(DIETS)2[Au(CN)4]", "2002", "", "RIKEN (The Institute of Physical and Chemical Research), 2-1 Hirosawa, Wako, Saitama, Japan", "J.Mater.Chem., 12(2002)159", "T.Imakubo,N.Tajima,M.Tamura,R.Kato,Y.Nishio,K.Kajita", "", "" ] }, { "id": "350", "line_start": 335, "line_end": 335, "sha256": "303794f49d3d5132c6363c0ce827219d3629c0bfb227e3b505281c1ab5246fd9", "values": [ "350", "PR05612905", "Cu[N(CN)2]Br", "kappa-(BEDT-TSF)2Cu[N(CN)2]Br", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.44", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "R = A*T^2. not SC.(metallic). dHvA effect measured down to 440 mK, 38.5 T.", "", "", "de Haas-van Alphen effect in the organic metal kappa-(BEDT-TSF)2Cu[N(CN)2]Br: Crossover to two-dimensional behavior in the complete-breakdown regime", "1997", "", "National High Magnetic Field Laboratory, LANL, Mailstop-E536, Los Alamos, New Mexico 87545", "Phys.Rev.B, 56(1997)12905", "N.Harrison,C.H.Mielke,D.G.Rickel,L.K.Montgomery,T.Burgin", "", "" ] }, { "id": "351", "line_start": 336, "line_end": 336, "sha256": "2327add52d0d2831e6b54ff40c2ecfdbbe86af00f689c92d61d57d32b624b01d", "values": [ "351", "CL19871819", "(CH3)4N", "[(CH3)4N][Ni(dmit)2]2", "", "Ni(dmit)2", "13.675", "6.476", "36.048", "", "94.74", "", "5", "5", "0.7", "0.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "dTc/dP)>0. thermal expansion coeff. alpha(a) = 7.7E-5/K, alpha(b) = 3.2 E-5/K, alpha = 2.5 E-5/K.", "", "", "The first molecular superconductor based on pai-acceptor molecules and closed-shell cations, [(CH3)4N][Ni(dmit)2]2, low temperature X-ray studies and superconducting transition", "1987", "", "", "Chem.Lett., (1987)1819-1822", "A.Kobayashi,H.Kim,Y.Sasaki,R.Kato,H.Kobayashi,S.Moriyama,Y.Nishio,K.Kajita,W.Sasaki", "", "" ] }, { "id": "352", "line_start": 337, "line_end": 337, "sha256": "3de40c1b8e7e95c7f490a7ea8b8a0646815f554595fc19c38a0c3966c75bcf3b", "values": [ "352", "CL19912163", "Me4N", "beta-[Me4N][Pd(dmit)2]2", "", "Pd(dmit)2", "14.541", "6.329", "35.136", "", "90.98", "", "6.2", "6.2", "0.65", "0.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3. space-G = C2/c. M-I transition at about 30 K under low pressure.", "", "", "New molecular superconductor, beta-[(CH3)4N][Pd(dmit)2]2", "1991", "", "", "Chem.Lett., (1991)2163-2166", "A.Kobayashi,H.Kobayashi,A.Miyamoto,R.Kato,R.A.Clark,A.E.Underhill", "", "" ] }, { "id": "353", "line_start": 338, "line_end": 338, "sha256": "70cd2d198f176eaea79b111ce033f7ec4137796697810e5e6f5ac7df7207c8db", "values": [ "353", "CL19931235", "EDT-TTF", "alpha-(EDT-TTF)[Ni(dmit)2]", "", "Ni(dmit)2", "", "", "", "", "", "", "1.3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "donor acceptor type. resistivity peak at 12 K. I//ab-plane. beta-type crystal is semiconductor.", "", "", "First ambient-pressure superconductor based on Ni(dmit)2, alpha-EDT-TTF[Ni(dmit)2]", "1993", "", "", "Chem.Lett., (1993)1235-1238", "H.Tajima,M.Inokuchi,A.Kobayashi,T.Ohta,R.Kato,H.Kobayashi,H.Kuroda", "", "" ] }, { "id": "354", "line_start": 339, "line_end": 339, "sha256": "5cb245cc58521da1df30d9a5e0b48f21c7c699b715720f5e385f97162fd69404", "values": [ "354", "SSC0650361", "(CH3)4N", "[(CH3)4N][Ni(dmit)2]2", "", "Ni(dmit)2", "", "", "", "", "", "", "5", "5", "0.7", "0.32", "", "", "", "7.9", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "(dTc/dP) calculated from the Tc values of P=0.7 and 0.32 GPa. resistivity anomaly at about 100K.", "", "", "Transport properties of ((CH3)4N)(Ni(dmit)2)2: A new organic superconductor", "1988", "", "", "Solid State Commun., 65(1988)361", "K.Kajita,Y.Nishio,S.Moriyama,R.Kato,H.Kobayashi,W.Sasaki,A.Kobayashi,H.Kim,Y.Sasaki", "", "" ] }, { "id": "355", "line_start": 340, "line_end": 340, "sha256": "d52fb0eb97152b07324320c3cc043947ccc7bb7a369a51dd4f5348ac100a807f", "values": [ "355", "ACS1234174", "SbF6", "beta-(BDA-TTP)2SbF6", "", "BDA-TTP", "8.579", "17.636", "6.514", "93.79", "110.75", "89", "6.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "resistive Tc = 7.5 K. form = C24H24S16SbF6.", "", "", "New Organic Superconductors beta-(BDA-TTP)2X : X = SbF6, AsF6, and PF6", "2001", "", "Faculty of Science, Himeji Institute of Technology, 3-2-1 Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan", "J.Am.Chem.Soc., 123(2001)4174", "J.Yamada,M.Watanabe,H.Akutsu,S.Nakatsuji,H.Nishikawa,I.Ikemoto,K.Kikuchi", "", "" ] }, { "id": "356", "line_start": 341, "line_end": 341, "sha256": "398c786235784c1d9bb572e65a854f19ed22bf1b19c9b718555c81717cd3e148", "values": [ "356", "ACS1234174", "AsF6", "beta-(BDA-TTP)2AsF6", "", "BDA-TTP", "8.523", "17.449", "6.518", "93.95", "110.74", "89.13", "5.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "resistive Tc = 5.8 K. form = C24H24S16AsF6", "", "", "New Organic Superconductors beta-(BDA-TTP)2X : X = SbF6, AsF6, and PF6", "2001", "", "Faculty of Science, Himeji Institute of Technology, 3-2-1 Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan", "J.Am.Chem.Soc., 123(2001)4174", "J.Yamada,M.Watanabe,H.Akutsu,S.Nakatsuji,H.Nishikawa,I.Ikemoto,K.Kikuchi", "", "" ] }, { "id": "357", "line_start": 342, "line_end": 342, "sha256": "90e6366f35a24ded3b6dc5360081837052b891f82c518c8ba147e20a8dcd3c60", "values": [ "357", "ACS1234174", "PF6", "beta-(BDA-TTP)2PF6", "", "BDA-TTP", "8.503", "17.34", "6.533", "94.07", "110.73", "89.36", "5.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "form = C24H24S16PF6", "", "", "New Organic Superconductors beta-(BDA-TTP)2X : X = SbF6, AsF6, and PF6", "2001", "", "Faculty of Science, Himeji Institute of Technology, 3-2-1 Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan", "J.Am.Chem.Soc., 123(2001)4174", "J.Yamada,M.Watanabe,H.Akutsu,S.Nakatsuji,H.Nishikawa,I.Ikemoto,K.Kikuchi", "", "" ] }, { "id": "358", "line_start": 343, "line_end": 343, "sha256": "b49cc14b8d3e66e6e661ce0d527bb6d8d16ebb8ca9180df581db4194aed3fcbe", "values": [ "358", "ACS1240730", "AsF6", "beta''-(DODHT)AsF6", "", "DODHT", "", "", "", "", "", "", "3.3", "", "", "1.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc decreases with increasing H at P=16.5 kbar. conductivity(300K) = 1.2 S/cm", "", "", "New Organic Superconductors Consisting of an Unprecedented pai-Electron Donor", "2002", "", "Department of Chemistry, Graduate School of Science, Tokyo Metropolitan UniVersity, Hachioji, Tokyo 192-0397, Tokyo", "J.Am.Chem.Soc., 124(2002)730", "H.Nishikawa,T.Morimoto,T.Kodama,I.Ikemoto,K.Kikuchi,J.Yamada,H.Yoshino,K.Murata", "", "" ] }, { "id": "359", "line_start": 344, "line_end": 344, "sha256": "a1eaa0f1ed67779b51a19da24f8bca380dc9a0c1078c604fab0362ec3cfe8d7f", "values": [ "359", "ACS1240730", "PF6", "beta''-(DODHT)PF6", "", "DODHT", "", "", "", "", "", "", "3.1", "", "", "1.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc disappears at H = 1 T under P=16.5 kbar. conductivity(300K) = 0.92 S/cm", "", "", "New Organic Superconductors Consisting of an Unprecedented pai-Electron Donor", "2002", "", "Department of Chemistry, Graduate School of Science, Tokyo Metropolitan UniVersity, Hachioji, Tokyo 192-0397, Tokyo", "J.Am.Chem.Soc., 124(2002)730", "H.Nishikawa,T.Morimoto,T.Kodama,I.Ikemoto,K.Kikuchi,J.Yamada,H.Yoshino,K.Murata", "", "" ] }, { "id": "360", "line_start": 345, "line_end": 345, "sha256": "fdd2f8283d19286027c754935336fb58dec012ef81e60748dfb0e623e4fb6d13", "values": [ "360", "CC20030494", "BF4:H2O", "beta''-(DODHT)2BF4:H2O", "", "DODHT", "5.8088", "16.095", "17.193", "72.109", "87.783", "86.951", "3.2", "", "", "1.55", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC disappear at H=1.6 T under P=15.5 kbar. triclinic. formula = C40H44S24O10B2F8", "", "", "A new organic superconductor, (DODHT)2BF4:H2O", "2003", "", "Department of Chemistry, Graduate School of Science, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan.", "Chem.Commun., (2003)494-495", "H.Nishikawa,A.Machida,T.Morimoto,K.Kikuchi,T.Kodama,I.Ikemoto,J.Yamada,H.Yoshino,K.Murata", "", "" ] }, { "id": "361", "line_start": 346, "line_end": 346, "sha256": "b8d6b7a7393da5cffc35b521ae0e8eeba4823b73eba19a9b6bc52d34ad68e593", "values": [ "361", "CC20032230", "GaCl4", "beta-(BDA-TTP)2GaCl4", "", "BDA-TTP", "12.4693", "38.768", "7.735", "", "91.199", "", "3.1", "", "", "0.76", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "hydrostatic pressure. conductivity(RT) = 53 S/cm. M-I transition at 118 K.", "", "", "A new organic superconductor, beta-(BDA-TTP)2GaCl4 [BDA-TTP = 2,5-(1,3-dithian-2-ylidene)-1,3,4,6-tetrathiapentalene]", "2003", "", "Department of Material Science, Graduate School of Science, Himeji Institute of Technology, 3-2-1 Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan.", "Chem.Commun., (2003)2230-2231", "J.Yamada,T.Toita,H.Akutsu,S.Nakatsuji,H.Nishikawa,I.Ikemoto,K.Kikuchi,F.S.Choi,D.Graf,J.S.Brooks", "", "" ] }, { "id": "362", "line_start": 347, "line_end": 347, "sha256": "a92fd419211105074d7b5f1fa1ec339e5b8e805dd7d05880a69a91faf8d778c1", "values": [ "362", "CC20042454", "PF6", "beta-(meso-DMBEDT-TTF)2PF6", "", "DMBEDT-TTF", "9.115", "15.649", "6.737", "90.84", "109.37", "88.87", "4.3", "", "", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "hydrostatic pressure. Tc(mid) = 3.8 K at P=4.0 kbar. M-I transition at 90 K. formula = C24H24S16PF6.", "", "", "A new organic superconductor beta-(meso-DMBEDT-TTF)2PF6", "2004", "", "The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan.", "Chem.Commun., (2004)2454-2455", "S.Kimura,T.Maejima,H.Suzuki,R.Chiba,H.Mori,T.Kawamoto,T.Mori,H.Moriyama,Y.Nishio,K.Kajita", "", "" ] }, { "id": "363", "line_start": 348, "line_end": 348, "sha256": "b9dc6386e1214b44837349d960e94ce16de152a14fbff7ed830447a17cb6b805", "values": [ "363", "CC20061592", "[Au(CN)4](THF)", "kappa-(DMEDO-TSeF)2[Au(CN)4](THF)", "", "DMEDO-TSeF", "38.868", "11.1527", "8.2788", "", "95.033", "", "4.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "R decreases monotonously with decreasing T. Tc(sus) = 4.6 K. space-G = P2<1>/c. monoclinic, formula = C28H28AuN4O5Se8.", "", "", "New ambient pressure organic superconductors k- and k-(DMEDOTSeF)2[Au(CN)4](THF)", "2006", "", "RIKEN, 2-1 Hirosawa, Wako, Saitama, 351-0198, Japan.", "Chem.Commun., (2006)1592-1594", "T.Shirahata,M.Kibune,T.Imakubo", "", "" ] }, { "id": "364", "line_start": 349, "line_end": 349, "sha256": "37c1c46ad3b3764b2037a9cf5107ed07e1c4024d8a5271e1891c66cf5c58b073", "values": [ "364", "CC20061592", "[Au(CN)4](THF)", "kappa-(DMEDO-TSeF)2[Au(CN)4](THF)", "", "DMEDO-TSeF", "8.3269", "38.638", "11.1203", "", "", "", "3", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "R shows broad maximum around 110K. Tc(sus) = 2.8 K. orth-. formula = C28H28AuN4O5Se8.", "", "", "New ambient pressure organic superconductors k- and k-(DMEDOTSeF)2[Au(CN)4](THF)", "2006", "", "RIKEN, 2-1 Hirosawa, Wako, Saitama, 351-0198, Japan.", "Chem.Commun., (2006)1592-1594", "T.Shirahata,M.Kibune,T.Imakubo", "", "" ] }, { "id": "365", "line_start": 350, "line_end": 350, "sha256": "e1df8fc2a08c6a7eed248492681092c9005a4b5f45391c73cb59e968cec81de7", "values": [ "365", "CL19880865", "Et2Me2N", "alpha-Et2Me2N[Ni(dmit)2]2", "", "Ni(dmit)2", "38.95", "6.494", "13.835", "", "99.63", "", "", "", "", "", "", "", "", "", "1.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3, Et=C2H5. not SC down to 1.5 K under P=5 kbar. monoclinic, space-G = C2/c.", "", "", "Crystal and electronic structures of a new two-dimensional molecular metal, alpha-Et2Me2N[Ni(dmit)2]2", "1988", "", "Toho University,Funabashi, Chiba", "Chem.Lett., (1988)865-868", "R.Kato,H.Kobayashi,H.Kim,A.Kobayashi,Y.Sasaki,T.Mori,H.Inokuchi", "", "" ] }, { "id": "366", "line_start": 351, "line_end": 351, "sha256": "1fc1a18d489c3b24ddb8cc56851d40bbbedc746d6e427549e99e26cab3c41def", "values": [ "366", "CL19891839", "EDT-TTF", "alpha-(EDT-TTF)[Ni(dmit)2]", "", "Ni(dmit)2", "6.658", "7.626", "27.385", "93.23", "91.43", "119.29", "", "", "", "", "", "", "", "", "4.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC down to 4.2 K. conductivity(RT) = 100 S/cm. R has a peak at 14 K.", "", "", "New molecular conductors, alpha- and beta-(EDT-TTF)[Ni(dmit)2] metal with anomalous resistivity maximum vs semiconductor with mixed stacks", "1989", "", "Toho University,Funabashi, Chiba", "Chem.Lett., (1989)1839-1842", "R.Kato,H.Kobayashi,A.Kobayashi,T.Naito,M.Tamura,H.Tajima,H.Kuroda", "", "" ] }, { "id": "367", "line_start": 352, "line_end": 352, "sha256": "c99573ad04d0c61da2826b6e5f8854f9ddf41ee080721b123bd2da4f4b083a9b", "values": [ "367", "PR0423935", "TTF", "TTF[Ni(dmit)2]2", "", "Ni(dmit)2", "", "", "", "", "", "", "2", "2", "0.95", "0.575", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc = 1.91 K, dTc = 0.2 K for P=12.3 kbar. (dR/dP)/R0 = 0.33 /kbar for T=300K.", "", "", "Simultaneous competition and coexistence between charge-density waves and reentrant superconductivity in the pressure-temperature phase diagram of the molecular conductor TTF [Ni(dmit)2]2 (TTF is tetrathiafulvalene and dmit is the 1,3-dithia-2-thione-4,5-dithiolato group)", "1990", "", "Laboratoire de Physique des Solides, Batiment 510, Universite Paris-Sud, 91405 Orsay, France", "Phys.Rev.B, 42(1990)3935", "L.Brossard,M.Ribault,L.Valade,P.Cassoux", "", "" ] }, { "id": "368", "line_start": 353, "line_end": 353, "sha256": "9afd227c68ce42658211a01c6510ed4cb152296c5d1b06c7693ff9b9e9e37dd6", "values": [ "368", "P070024517", "FeCl4", "beta-(BDA-TTP)2FeCl4", "", "BDA-TTP", "", "", "", "", "", "", "2", "2", "0.63", "0.45", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "resistivity along b-axis.", "", "", "Pressure-dependent ground states and fermiology in beta-(BDA-TTP)2MCl4 (M=Fe,Ga)", "2004", "", "National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA", "Phys.Rev.B, 70(2004)024517", "E.S.Choi,D.Graf,J.S.Brooks,J.Yamada,H.Akutsu,K.Kikuchi,M.Tokumoto", "", "" ] }, { "id": "369", "line_start": 354, "line_end": 354, "sha256": "ce4add13dea697f066914048301cc90b03a46450475034d38087fe28c09355c2", "values": [ "369", "CL19921909", "Me2Et2N", "[Me2Et2N][Pd(dmit)2]2", "", "Pd(dmit)2", "8.218", "18.422", "6.277", "96.76", "115.7", "90.09", "4", "4", "0.24", "0.23", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Me=CH3, Et=C2H5. triclinic, space-G = P1[-]. conductivity(RT) = 80 S/cm. Tc(3.8 kbar) = 3.4 K.", "", "", "New molecular superconductor, [Me2Et2N][Pd(dmit)2]2", "1992", "", "Toho University,Funabashi, Chiba", "Chem.Lett., (1992)1909-1912", "H.Kobayashi,K.Bun,T.Naito,R.Kato,A.Kobayashi", "", "" ] }, { "id": "370", "line_start": 355, "line_end": 355, "sha256": "746096834800222ef77d40ffe4012f0f9ee8856fa449d39f4a57fb044b2107fd", "values": [ "370", "NAT4100908", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "0.85", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH370", "", "", "", "", "Field-induced SC. Tc defined as R/Rn = 0.5. M-I transition at 80 K for H = 0. Tc value shows for H//c-axis. CAN in figure represent \"canted antiferromagnetism\".", "OPH370.dat", "", "Magnetic-field-induced superconductivity in a two-dimensional organic conductor", "2001", "", "National Research Institute for Metals, Tsukuba,Ibaraki,Japan", "Nature, 410(2001)908", "S.Uji,H.Shinagawa,T.Terashima,T.Yakabe,Y.Terai,M.Tokumoto,A.Kobayashi,H.Tanaka,H.Kobayashi", "", "" ] }, { "id": "371", "line_start": 356, "line_end": 356, "sha256": "9e8fb25d7cf8e8b2a83ae87efc34ba67a0d932fe23ab2ffbaf509b9441932606", "values": [ "371", "INO0302586", "Cu2(CN)3", "kappa-(BEDT-TTF)2Cu2(CN)3", "", "BEDT-TTF", "16.117", "8.5858", "13.397", "", "113.42", "", "2.8", "", "", "0.15", "", "", "", "-12.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc by rf-impedance.", "", "", "Superconductivity at 2.8 K and 1.5 kbar in kappa-(BEDT-TTF)2Cu2(CN)3: The first organic superconducting a polymeric copper cyanide anion", "1991", "", "", "Inorg.Chem., 30(1991)2586", "U.Geiser,H.H.Wang,K.D.Carlson,J.M.Williams,H.A.Chrlier,Jr,J.E.Heindl,G.A.Yaconi,B.J.Love,M.W.Lathrop,J.E.Schirber,D.L.Overmyer,J.Ren,M-H.Whangbo", "", "" ] }, { "id": "372", "line_start": 357, "line_end": 357, "sha256": "26b567aba9f9d6915dd9401f24decccbac3c63979efe61f202a1c788b1156166", "values": [ "372", "SYN0610199", "AuI2", "(DMET-TSeF)2AuI2", "", "DMET-TSeF", "7.799", "15.869", "6.74", "98.16", "104.49", "89.48", "0.58", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "no M-I transition", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "373", "line_start": 358, "line_end": 358, "sha256": "960d1804ddaafb013232f27f3e54405548758a05bfcc6930dcace2ca08b98563", "values": [ "373", "SYN0610199", "AuBr2", "(DMET-TSeF)2AuBr2", "", "DMET-TSeF", "7.763", "15.788", "6.75", "101.39", "104.21", "91.08", "", "", "", "", "", "", "", "", "2.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC. resistivity minimum at 35 K. metallic resistivity for P>8kbar", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "374", "line_start": 359, "line_end": 359, "sha256": "28c6e85432b4ce35e9b5a0086e1df1c644fc0dae2e99d6b5df10e2a975d8b242", "values": [ "374", "SYN0610199", "AuCl2", "(DMET-TSeF)2AuCl2", "", "DMET-TSeF", "7.81", "15.174", "7.021", "90.83", "109.06", "79.79", "", "", "", "", "", "", "", "", "4.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "375", "line_start": 360, "line_end": 360, "sha256": "1c4f7348bdc8b39c1538ddfdfced906746f2c07a4c6a9b453a87bf16cdf96739", "values": [ "375", "SYN0610199", "Au(CN)2", "(DMET-TSeF)2Au(CN)2", "", "DMET-TSeF", "7.805", "15.402", "6.759", "96.02", "104.76", "87.91", "", "", "", "", "", "", "", "", "4.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "376", "line_start": 361, "line_end": 361, "sha256": "8d0c4a8a18149e4eb0da73e3ecf0a03f6fc373091a64c8caaaaf0398d93e3e2d", "values": [ "376", "SYN0610199", "I2", "(DMET-TSeF)2I2", "", "DMET-TSeF", "7.826", "15.908", "6.737", "97.79", "102.42", "89.55", "", "", "", "", "", "", "", "", "4.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC", "", "", "Metallic and superconducting salts based on an unsymmetrical pai-donor dimethyl(ethylenedithio)tetraselenafulvalene (DMET-TSeF)", "1993", "", "", "Synth.Met., 61(1993)199", "R.Kato,S.Aonuma,Y.Okano,H.Sawa,M.Tamura,M.Kinoshita,K.Oshima,A.Kobayashi,K.Bun,H.Kobayashi", "", "" ] }, { "id": "377", "line_start": 362, "line_end": 362, "sha256": "8e205dfd736fd102e66b05e5cf00778093864a029eb78818da2d0775cdb5ac36", "values": [ "377", "SYN0552927", "Me2Et2N", "Me2Et2N[Pd(dmit)2]2", "", "Pd(dmit)2", "8.218", "18.422", "6.277", "96.76", "115.7", "90.09", "4", "", "", "0.24", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC377", "", "", "", "", "CH3=Me, C2H5=Et. triclinic, P1[-]. Figure shows phase diagram.", "OTC377.dat", "", "New molecular superconductors, beta-[(CH3)4N][Pd(dmit)2]2 and [(CH3)2(C2H5)2N][Pd(dmit)2]2", "1993", "", "Department of Chemistry, Faculty of Science, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 116, Japan", "Synth.Met., 55-57(1993)2927", "A.Kobayashi,R.Kato,R.A.Clark,A.E.Underhill,A.Miyamoto,K.Bun,T.Naito,H.Kobayashi", "", "" ] }, { "id": "378", "line_start": 363, "line_end": 363, "sha256": "f34123ce17f07a662d81ec5c8302e5311bf1a496570f4bdf9d7ed5ae8792eefe", "values": [ "378", "SYN0552927", "Me4N", "beta-Me4N[Pd(dmit)2]2", "", "Pd(dmit)2", "14.541", "6.329", "35.136", "", "90.98", "", "6.3", "", "", "0.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC378", "", "", "", "", "CH3=Me. monoclinic. Figure shows phase diagram.", "OTC378.dat", "", "New molecular superconductors, beta-[(CH3)4N][Pd(dmit)2]2 and [(CH3)2(C2H5)2N][Pd(dmit)2]2", "1993", "", "Department of Chemistry, Faculty of Science, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 116, Japan", "Synth.Met., 55-57(1993)2927", "A.Kobayashi,R.Kato,R.A.Clark,A.E.Underhill,A.Miyamoto,K.Bun,T.Naito,H.Kobayashi", "", "" ] }, { "id": "379", "line_start": 364, "line_end": 364, "sha256": "a829e9d7101f8f979c78692c56ed082ce2c2a2aed7db0f38587d88472436ae56", "values": [ "379", "SYN027B157", "TTF", "alpha'-TTF[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "6.42", "6.42", "2.07", "1.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC379", "", "", "", "", "(dlogR/dP) = 0.10 /kbar. monoclinic. M-I transition at 220 K.", "OTC379.dat", "", "Pressure-temperature phase diagram of alpha'-TTF [Pd(Dmit)2]2", "1988", "", "Laboratoire de Physique des Solides, Universite Paris-Sud-91405, Orsay, France", "Synth.Met., 27(1988)B157", "L.Brossard,H.Hurdequint,M.Ribault,L.Valade,J.P.Legros,P.Cassoux", "", "" ] }, { "id": "380", "line_start": 365, "line_end": 365, "sha256": "cfc3d142ec3f92c5f9614be29c21051e8425d9d6cf8a613f21c6ef247f25d1a4", "values": [ "380", "SYN027B157", "TTF", "alpha'-TTF[Pd(dmit)2]2", "", "Pd(dmit)2", "", "", "", "", "", "", "5.93", "5.93", "2.42", "1.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "monoclinic. M-I transition at 220 K.", "", "", "Pressure-temperature phase diagram of alpha'-TTF [Pd(Dmit)2]2", "1988", "", "Laboratoire de Physique des Solides, Universite Paris-Sud-91405, Orsay, France", "Synth.Met., 27(1988)B157", "L.Brossard,H.Hurdequint,M.Ribault,L.Valade,J.P.Legros,P.Cassoux", "", "" ] }, { "id": "381", "line_start": 366, "line_end": 366, "sha256": "bd12e5e7e5983eb286015f7a1ad210f0e2642e05744a309cfb103348687695f3", "values": [ "381", "P075054509", "I3", "theta-(BEDT-TTF)2I3", "3", "BEDT-TTF", "9.929", "10.075", "34.2", "", "98.268", "", "3.6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "About 1/3 of measured crystals became SC below 3.6 K. space G = P2(1)/c.", "", "", "Electronic properties of the organic metals theta-(BEDT-TTF)2I3 and theta-(BEDT-TTF)2I3", "2007", "", "Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, 70050 Stuttgart, Germany", "Phys.Rev.B, 75(2007)054509", "B.Salameh,A.Nothardt,E.Balthes,W.Schmidt,D.Schweitzer,J.Strempfer,B.Hinrichsen,M.Jansen,D.K.Maude", "", "" ] }, { "id": "382", "line_start": 367, "line_end": 367, "sha256": "2f6eff71240f6d784f2fc092857b59a4e95c4388421361a1a4cfd11a703b8e26", "values": [ "382", "P075054509", "I3", "theta-(BEDT-TTF)2I3", "3", "BEDT-TTF", "9.964", "10.088", "34.419", "", "97.98", "", "5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Theta-phase changes to theta-phase after tempered at 70 K for 2h. All crystals are SC. Tc(on) = 7 K. space G = P2(1)/c.", "", "", "Electronic properties of the organic metals theta-(BEDT-TTF)2I3 and theta-(BEDT-TTF)2I3", "2007", "", "Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, 70050 Stuttgart, Germany", "Phys.Rev.B, 75(2007)054509", "B.Salameh,A.Nothardt,E.Balthes,W.Schmidt,D.Schweitzer,J.Strempfer,B.Hinrichsen,M.Jansen,D.K.Maude", "", "" ] }, { "id": "383", "line_start": 368, "line_end": 368, "sha256": "4f8a81421ba43771ee86476bbbc556cfd1207de381938cdf86690f81e21609aa", "values": [ "383", "J076033704", "EtMe3P", "EtMe3P[Pd(dmit)2]2", "3", "Pd(dmit)2", "", "", "", "", "", "", "4.8", "5.5", "0.2", "0.15", "", "", "", "", "", "4.4", "", "", "", "", "", "", "", "", "", "", "", "OTC383", "OHC383", "", "", "", "valence bond ordering temp, T shown in Fig. Hc1(T) shown in Fig. anisotropy factor from Hc1 = 4. Et=C2H5, Me=CH3.", "OTC383.dat", "OHC383.dat", "Magnetic Study of Pressure-Induced Superconductivity in the [Pd(dmit)2] Salt with Spin-Gapped Ground State", "2007", "", "Condensed Molecular Materials Laboratory, RIKEN, 2-1 Hirosawa, Wako, Saitama 351-1098", "J.Phys.Soc.Jpn, 76(2007)033704", "Y.Ishii,M.Tamura,R.Kato", "", "" ] }, { "id": "384", "line_start": 369, "line_end": 369, "sha256": "b99831ac4d3a7596daa0707c8c41916869ae11ee12d533c8ba3973d9c88fc010", "values": [ "384", "J076034709", "PF6", "beta''-(DODHT)2PF6", "", "DODHT", "5.7808", "9.2199", "15.784", "101.222", "98.469", "107.27", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "tricrinic. a=5.634, b=9.031, c=15.780,alpha=101.43, beta=98.23, gamma=106.39 for P=0.75 GPa. a=5.4273, b=8.650, c=15.76,alpha=101.54, beta=97.73, gamma=104.95 for P=1.9 GPa. P= hydrostatic pressure.", "", "", "Structural Studies of Pressure-Induced Organic Superconductor beta''-(DODHT)2PF6 Having Charge-Ordering Phase at Ambient Pressure", "2007", "", "Department of Basic Science, University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902", "J.Phys.Soc.Jpn, 76(2007)034709", "M.Higa,R.Kondo,S.Kagoshima,H.Nishikawa", "", "" ] }, { "id": "385", "line_start": 370, "line_end": 370, "sha256": "91bce3054877e38d7fa974a593a55b352340a7241809e60caf859a11306a769c", "values": [ "385", "ASP3020205", "TTF", "TTF[Ni(dmit)2]2", "", "Ni(dmit)2", "46.22", "3.732", "22.86", "", "119.29", "", "1.62", "", "", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "(dTc) = 0.57 K. space-G = C2/c.", "", "", "Physique de la matiere condensee (chimie de coordination). - Un nouveau type de supraconducteur moleculaire: TTF[Ni(dmit)2]2", "1986", "", "", "C.R.Acad.Sci.Paris,Ser.II 302(1986)205", "L.Brossard,M.Ribault,M.Bousseau,L.Valade,P.Cassoux", "", "" ] }, { "id": "386", "line_start": 371, "line_end": 371, "sha256": "963b29f9f76ce92221aef9c723df59f35d362fcfd1f574e157b239232a3a07bf", "values": [ "386", "EP07837005", "TTF", "TTF[Ni(dmit)2]2", "", "Ni(dmit)2", "", "", "", "", "", "", "0.8", "", "", "0.77", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Film. films were electrodeposited on (001)Si plate. fiber-like morphology(a-c in plane). Tc defined as Tc(on). R(0.08K)/R(Tc) = 0.935.", "", "", "Superconductivity in TTF[Ni(dmit)2]2 films", "2007", "", "Laboratoire de Chimie de Coordination, UPR CNRS 8241 - 205 route de Narbonne, F-31077 Toulouse, France", "Europhys.Lett., 78(2007)37005", "J.-P.Savy,D.de Caro,L.Valade,J.-P.Legros,P.Auban-Senzier,C.R.Pasquier,J.Fraxedas,F.Senocq", "", "" ] }, { "id": "387", "line_start": 372, "line_end": 372, "sha256": "202395d80a7dc17542916f09752f1e078315acb1338425b19ddcce2f65cc9294", "values": [ "387", "J076053703", "AsF6", "(TMTTF)2AsF6", "3", "TMTTF", "", "", "", "", "", "", "2.3", "", "", "4.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC region: 0.45=< SC =<5.0 GPa. For P = 0, spin-peiels state and MI transition T = 140 K. Crystals grown by electro-crystallization method.", "", "", "Pressure-Induced Superconductivity in the Quasi-One-Dimensional Organic Conductor (TMTTF)2AsF6", "2007", "", "Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581", "J.Phys.Soc.Jpn, 76(2007)053703", "M.Itoi,M.Kano,N.Kurita,M.Hedo,Y.Uwatoko,T.Nakamura", "", "" ] }, { "id": "388", "line_start": 373, "line_end": 373, "sha256": "3ae47187c957cacd27fdd9a45c74fdf9f1df3bde33091a5dd801115a53e03618", "values": [ "388", "CC20042454", "PF6", "beta-(meso-DMBETT-TTF)2PF6", "", "DMBETT-TTF", "9.115", "15.649", "6.737", "90.84", "109.37", "88.87", "3.8", "", "", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "space-G = P1[-]. XRD at 293 K. formula = C24H24F6PS16. molar weight = 970.38. MI transition T = 90 K. Tc(on) = 4.3 K at P=4.0 kbar.", "", "", "A new organic superconductor beta-(meso-DMBEDT-TTF)2PF6", "2004", "", "The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan.", "Chem.Commun., (2004)2454-2455", "S.Kimura,T.Maejima,H.Suzuki,R.Chiba,H.Mori,T.Kawamoto,T.Mori,H.Moriyama,Y.Nishio,K.Kajita", "", "" ] }, { "id": "389", "line_start": 374, "line_end": 374, "sha256": "21c6ac000640e7308eb97f91e263ad652c88fdcc67ffc4919ed54449962f90ff", "values": [ "389", "L088207002", "PF6", "(TMTSF)2PF6", "3", "TMTSF", "", "", "", "", "", "", "1.18", "", "", "0.55", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC389", "", "", "", "", "Hc2(T) for H//c was measured. penet = 100 um for H//c is refered from SSC0450767.", "OHC389.dat", "", "Critical Field Enhancement near a Superconductor-Insulator Transition", "2002", "", "Department of Physics, Princeton University, Princeton, New Jersey 08544", "Phys.Rev.Lett., 88(2002)207002", "I.J.Lee,P.M.Chaikin,M.J.Naughton", "", "" ] }, { "id": "390", "line_start": 375, "line_end": 375, "sha256": "464def6eed04b96bc3dedc2f4db0d49f5466c5cef4e8df9c7e67f1d8f39a196e", "values": [ "390", "CC20061331", "I3", "beta-(BDA-TTP)2I3", "3", "BDA-TTP", "9.246", "16.792", "6.495", "95.263", "106.576", "95.766", "10.5", "", "", "1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc defined as Tc(on) resistively. SC confirmed by SUS. activation energy = 54 meV. hydrostatic pressure. space-G = P1[-]. molar weight = 1206.13. formula = C24H24I3S16.", "", "", "Pressure effect on the electrical conductivity and superconductivity of beta-(BDA-TTP)2I3", "2006", "", "Department of Material Science, Graduate School of Material Science, University of Hyogo, 3-2-1 Kouto, Kamigori-cho, Ako-gun, Hyogo, Japan", "Chem. Commun., (2006)1331", "J.Yamada,K.Fujimoto,H.Akutsu,S.Nakatsuji,A.Miyazaki,M.Aimatsu,S.Kudo,T.Enoki,K.Kikuchi", "", "" ] }, { "id": "391", "line_start": 376, "line_end": 376, "sha256": "0a502e0b03070ad170c89d60a43326ddc68197f73a101e970a6246ac8a60bd68", "values": [ "391", "L096177002", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(SCN)2", "3", "BEDT-TTF", "", "", "", "", "", "", "10.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC391", "", "", "", "", "Defects created at RT by Cu-K radiation, flux = 2.5 E+8 photon/s. Figure shows Tc vs residual resistivity( radiation effect)", "OTC391.dat", "", "Effect of Irradiation-Induced Disorder on the Conductivity and Critical Temperature of the Organic Superconductor kappa-(BEDT-TTF)2Cu(SCN)2", "2006", "", "Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom", "Phys.Rev.Lett., 96(2006)177002", "J.G.Analytis,A.Ardavan,S.J.Blundell,R.L.Owen,E.F.Garman,C.Jeynes,B.J.Powell", "", "" ] }, { "id": "392", "line_start": 377, "line_end": 377, "sha256": "e20a7fea4206f5603ce46d2bae18fde3ccc896a8084ef037381ea9fbd97f7df2", "values": [ "392", "JPP0501521", "TTF", "alpha'-TTF(Pd(dmit)2)2", "3", "Pd(dmit)2", "46.794", "3.608", "23.109", "90", "119.55", "90", "6.53", "6.53", "2.07", "1.6", "", "", "", "", "", "", "0.102", "0.0217", "", "", "", "", "", "", "", "", "", "OHC392", "", "", "", "", "SC properties for P = 2.07 GPa. H // a-axis.", "OHC392.dat", "", "Pressure induced superconductivity in molecular TTF(Pd(dmit)2)2", "1989", "", "", "J.Phys.France, 50(1989)1521", "L.Brossard,M.Ribault,L.Valade,P.Cassoux", "", "" ] }, { "id": "393", "line_start": 378, "line_end": 378, "sha256": "0b0898528a1ad82fed88e63387d62c583d89ffad9007ff12683fbcf2113b40fc", "values": [ "393", "JPI0041539", "Br", "(TMTTF)2Br", "3", "TMTTF", "", "", "", "", "", "", "0.8", "", "", "2.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "15", "", "", "", "", "", "Tc defined as R/Rn = 0.5. dTc = 0.4 K. Tc(on) = 1.0 K. SDW transition at 15 K(P=AP) and 4 K (P=24 kbar).", "", "", "Superconductivity and magnetic field induced spin density waves in the (TMTTF)2X family", "1994", "", "", "J.Phys.I France, 4(1994)1539", "L.Balicas,K.Behnia,W.Kang,E.Canadell,P.Auban-Senzier,D.Jerome,M.Ribault,J.M.Fabre", "", "" ] }, { "id": "394", "line_start": 379, "line_end": 379, "sha256": "a6a6475ea5f932d12f8729173693cdebff31d17030f769fcf2ad484bb2fb12e3", "values": [ "394", "MOL2960217", "Me4Sb", "beta'-Me4Sb[Pd(dmit)2]2", "3", "Pd(dmit)2", "14.356", "6.404", "36.893", "", "97.54", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC under (P=15 kbar, T=9 K or P=9.7 kbar, T=3 K). Me = CH3. space-G = C2/c.", "", "", "Se-substitution and cation effects on the high-pressure molecular superconductor, beta-Me4N[Pd(dmit)2]2 - A unique two-band system -", "1997", "", "The Institute for Solid State Physics, The University of Tokyo, Japan", "Mol.Cryst.Liq.Cryst., 296(1997)217", "R.Kato,Y.L. Liu,Y.Kobayashi,S.Aonuma", "", "" ] }, { "id": "395", "line_start": 380, "line_end": 380, "sha256": "156522381cd1ae721ecff27275384333ca439380cd1c00d3988e27b7bfd8a313", "values": [ "395", "MAT0303315", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "10.4", "", "", "0", "", "", "", "", "", "", "30", "", "", "", "", "", "", "", "", "", "", "OHC395", "", "", "", "", "Hc2=30 (TBL value) and 5 T for H// and H/n to conduction plane at T = 90 mK . Figure shows Hc2(T) at P = 1.75 GPa. paramagnetic limit Hc2 = 18 T.", "OHC395.dat", "", "Critical field and Shubnikov-de Haas oscillations of kappa-(BEDT-TTF)2Cu(NCS)2under pressure", "2003", "", "Department of Physics, Clark University, 950 Main St., Worcester, MA 01610", "cond. mat., 0303315(2003)", "C.Martin,C.C.Agosta,S.W.Tozer,H.A.Radovan,T.Kinoshita,M.Tokumoto", "", "" ] }, { "id": "396", "line_start": 381, "line_end": 381, "sha256": "2c6cb269b5a7c9e5fba347940c7be3f2c5ea21bcc4f62536d08f383f65a8de89", "values": [ "396", "JP012L641", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "10.4", "", "", "0", "", "", "", "", "", "", "35", "", "", "", "", "", "", "", "", "", "", "OHC396", "", "", "", "", "Figure shows phase diagram Hc2(T),mixed state, FFLO state.", "OHC396.dat", "", "Observation of the Fulde-Ferrell-Larkin-Ovchinnikov state in the quasi-two-dimensional organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 (BEDT-TTF = bis(ethylene-dithio)tetrathiafulvalene)", "2000", "", "Department of Physics, University of Oxford, The Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UK", "J.Phys.:Condens.Matter, 12(2000)L641", "J.Singleton,J.A.Symington,M-S.Nam,A.Ardavan,M.Kurmoo,P.Day", "", "" ] }, { "id": "397", "line_start": 382, "line_end": 382, "sha256": "0865f12dc5365b75ffc67c35c5aea6ed71eb9d8a8be30b09e7da792b55e0ac82", "values": [ "397", "SUP0120497", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "9.4", "", "", "0", "", "", "", "", "", "", "5.2", "", "", "", "", "", "", "", "", "", "", "OHC397", "", "", "", "", "Hc2 measured by microwave, thermal conductivity, and resistivity.", "OHC397.dat", "", "Probing the Upper Critical Field of kappa-(BEDT-TTF)2Cu(NCS)2", "1999", "", "Laboratoire de Physique des Solides (CNRS), Universite Paris- Sud, F-91405 Orsay, France", "J.Supercond., 12(1999)497", "S.Belin,T.Shibauchi,K.Behnia,T.Tamegai", "", "" ] }, { "id": "398", "line_start": 383, "line_end": 383, "sha256": "7c8501beefe06f36f6685aa1a0a27c449838a6cc411d44f7205cf576b1c39fda", "values": [ "398", "SUP0120501", "NH4Hg(SCN)4", "alpha-(BEDT-TTF)2NH4Hg(SCN)4", "3", "BEDT-TTF", "", "", "", "", "", "", "1.3", "", "", "0", "", "", "", "", "", "", "5.5", "", "", "", "", "", "", "", "", "", "", "OHC398", "", "", "", "", "Prepared by electro chemical method(1.5*0.8*0.5 mm3). Hc2 measured for H//a and defined as R(on).", "OHC398.dat", "", "Superconducting State of the Two-Dimensional Superconductor alpha-(ET)2NH4Hg(SCN)4 Under the Magnetic Field Parallel to the Conducting Plane", "1999", "", "Department of Physics, Kyoto University, Kyoto 606-8502, Japan", "J.Supercond., 12(1999)501", "Y.Shimojo,H.Ito,T.Ishiguro,T.Kondo,G.Saito", "", "" ] }, { "id": "399", "line_start": 384, "line_end": 384, "sha256": "52dfa54da90534041c1eb7c31d375b03785265c5b5e6535437628b74298a2944", "values": [ "399", "SUP0120511", "GaCl4", "ramda-(BETS)2GaCl4", "3", "BETS", "", "", "", "", "", "", "6.2", "", "", "0", "", "", "", "", "", "", "14", "2.8", "104", "", "", "", "", "", "", "", "", "OHC399", "", "", "", "", "Tc, Hc2 defined as R/Rn = 0.5. Hc2(0) = 14, 3.5, 12.3 T and (dHc2/dT) = 2.8, 0.36, 2.8 T/K for a*-, b*-, c-axis , respectively. cohere = 104, =26, =91 A estimated from Hc2(0).", "OHC399.dat", "", "Anisotropy of the Upper Critical Field of the Organic Superconductor ramda-(BETS)2GaCl4", "1999", "", "Department of Physics, Kyoto University, Kitashirakawa, Sakyoku, Kyoto 606-8502, Japan", "J.Supercond., 12(1999)511", "M.A.Tanatar,T.Ishiguro,H.Tanaka,A.Kobayashi,H.Kobayashi", "", "" ] }, { "id": "400", "line_start": 385, "line_end": 385, "sha256": "d925208e1d4f92937bbdb779170047661e6507eed02510f8bd188e76821cac64", "values": [ "400", "PR04104808", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "9.4", "", "", "0", "", "", "", "", "", "", "", "16", "", "", "", "", "", "36", "", "", "", "", "", "", "", "", "Hc2 measured by SP-heat. -(dHc2/dT) = 0.75 T/K for H//a and = 16 T/K for H//b-c plane. (dC/gamma*Tc) = 1.50.", "", "", "Specific heat of superconducting kappa-(BEDT-TTF)2Cu(NCS)2 near Tc [where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene]", "1990", "", "AT&T Bell Laboratories, Murray Hill, New Jersey 07974", "Phys.Rev.B, 41(1990)4808", "J.E.Graebner,R.C.Haddon,S.V.Chichester,S.H.Glarum", "", "" ] }, { "id": "401", "line_start": 386, "line_end": 386, "sha256": "b0a6f2eabf59b88273148aabf7213f7ccc1c48ea34078cc119f1744bfe426977", "values": [ "401", "P076054509", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "11.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "sound velocity, ultrasonic attenuation were measured.", "", "", "Competition between magnetism and superconductivity in the organic metal kappa-[BEDT-TTF]2Cu[N(CN)2]Br", "2007", "", "Regroupement Quebecois sur les Materiaux de Pointe, Departement de Physique, Universite de Sherbrooke, Sherbrooke, Quebec, Canada", "Phys.Rev.B, 76(2007)054509", "D.Fournier,M.Poirier,K.D.Truong", "", "" ] }, { "id": "402", "line_start": 387, "line_end": 387, "sha256": "b1855b820ba43bfc64be688bff094dba5b069c0a8cfe7dbf82da4f35203b4735", "values": [ "402", "J076113709", "Hg2.89Br8", "kappa-(BEDT-TTF)4Hg2.89Br8", "3", "BEDT-TTF", "", "", "", "", "", "", "4.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC402", "", "", "", "", "single crystal by electrochemical mathod. Hydrostatic P upto 3.3 GPa. I// and /* to plane, measured. Figure shows Tc(P) as the same symbol for all samples", "OTC402.dat", "", "Anomalous Pressure Dependence of Superconductivity in Layered Organic Conductor, kappa-(BEDT-TTF)4Hg2:89Br8", "2007", "", "Department of Physics, Faculty of Science, Saitama University, Saitama 338-8570", "J.Phys.Soc.Jpn, 76(2007)113709", "H.Taniguchi,T.Okuhata,T.Nagai,K.Satoh,N.Mori,Y.Shimizu,M.Hedo,Y.Uwatoko", "", "" ] }, { "id": "403", "line_start": 388, "line_end": 388, "sha256": "c90a7fd89377a3dd8d1a88ed54a0fd62715799eee400f5d0a68fd97409fa1e69", "values": [ "403", "SSC0870589", "Cu[N(CN)2](Cl,Br)", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl0.85Br0.15", "3", "BEDT-TTF", "", "", "", "", "", "", "12.8", "12.8", "0.02", "0.008", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC403", "", "", "", "", "", "OTC403.dat", "", "Pressure effect on superconductivity in the organic crystal family kappa-(BEDT-TTF)2Cu[N(CN)2]Cl1-xBrx", "1993", "", "Walther-Meissner-Institute for low-temperature Research, W-8046 Garching, Germany", "Solid State Commun., 87(1993)589", "Yu.V.Sushko,K.Andres,N.D.Kusch,E.B.Yagubskii", "", "" ] }, { "id": "404", "line_start": 389, "line_end": 389, "sha256": "45858f79609bf0a0ece32dcb265376660f8ab692c9f9dbc9f927b2b838d693da", "values": [ "404", "SSC0870589", "Cu[N(CN)2](Cl,Br)", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl0.8Br0.2", "3", "BEDT-TTF", "", "", "", "", "", "", "13", "13", "0.025", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC404", "", "", "", "", "", "OTC404.dat", "", "Pressure effect on superconductivity in the organic crystal family kappa-(BEDT-TTF)2Cu[N(CN)2]Cl1-xBrx", "1993", "", "Walther-Meissner-Institute for low-temperature Research, W-8046 Garching, Germany", "Solid State Commun., 87(1993)589", "Yu.V.Sushko,K.Andres,N.D.Kusch,E.B.Yagubskii", "", "" ] }, { "id": "405", "line_start": 390, "line_end": 390, "sha256": "286d06c6cb293881bd6b847442ec3236f7f190cbc83e106d6059d73f375b3dc0", "values": [ "405", "SSC0870589", "Cu[N(CN)2](Cl,Br)", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl0.7Br0.3", "3", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC405", "", "", "", "", "", "OTC405.dat", "", "Pressure effect on superconductivity in the organic crystal family kappa-(BEDT-TTF)2Cu[N(CN)2]Cl1-xBrx", "1993", "", "Walther-Meissner-Institute for low-temperature Research, W-8046 Garching, Germany", "Solid State Commun., 87(1993)589", "Yu.V.Sushko,K.Andres,N.D.Kusch,E.B.Yagubskii", "", "" ] }, { "id": "406", "line_start": 391, "line_end": 391, "sha256": "5428d67fe4d9a667ee61befbbc1d6b02aa88277bef536d8ea06f31c86d165424", "values": [ "406", "SSC0870589", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC406", "", "", "", "", "", "OTC406.dat", "", "Pressure effect on superconductivity in the organic crystal family kappa-(BEDT-TTF)2Cu[N(CN)2]Cl1-xBrx", "1993", "", "Walther-Meissner-Institute for low-temperature Research, W-8046 Garching, Germany", "Solid State Commun., 87(1993)589", "Yu.V.Sushko,K.Andres,N.D.Kusch,E.B.Yagubskii", "", "" ] }, { "id": "407", "line_start": 392, "line_end": 392, "sha256": "65782772edee5212eeedb77d47b5f1a433876ff2307a0b2b7c367c2d7222a317", "values": [ "407", "L099057001", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "12.25", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "28", "", "", "", "", "", "", "", "", "SP-heat using long relaxation method. gamma is saturated value for high magnetic field (P>8T). alpha=1.7 (d-wave alpha-model)", "", "", "Specific-Heat Measurements of the Gap Structure of the Organic Superconductors kappa-(ET)2Cu[N(CN)2]Br and kappa-(ET)2Cu(NCS)2", "2007", "", "H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol, United Kingdom.", "Phys.Rev.Lett., 99(2007)057001", "O.J.Taylor,A.Carrington,J.A.Schlueter", "", "" ] }, { "id": "408", "line_start": 393, "line_end": 393, "sha256": "6e6acc0920baa46ed4af9ee54d43415744cee331f9f45c5e1cfe6ac51863e747", "values": [ "408", "L099057001", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.56", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "35", "", "", "", "", "", "", "", "", "SP-heat using long relaxation method. gamma is saturated value for high magnetic field (P > 3T). alpha=1.4 (d-wave alpha-model).", "", "", "Specific-Heat Measurements of the Gap Structure of the Organic Superconductors kappa-(ET)2Cu[N(CN)2]Br and kappa-(ET)2Cu(NCS)2", "2007", "", "H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol, United Kingdom.", "Phys.Rev.Lett., 99(2007)057001", "O.J.Taylor,A.Carrington,J.A.Schlueter", "", "" ] }, { "id": "409", "line_start": 394, "line_end": 394, "sha256": "a453036cd798b92cf7bc09462e823186845468779d4d379c6449f46027a32778", "values": [ "409", "PLA1200087", "TTF", "TTF[Ni(dmit)2]2", "3", "Ni(dmit)2", "", "", "", "", "", "", "1.62", "1.62", "0.7", "0.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC409", "", "", "", "", "Tc defined as onset of ESR.", "OTC409.dat", "", "EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF TETRATHIOFULVALENE BIS- [ BIS- (4,5-DIMERCAPTO 1,3-DITHIOL-2-THIONE) NICKEL (II)] (TTF[Ni(DMIT)2]2)", "1987", "", "Sandia National Laboratories, Albuquerque, NM 87185, USA", "Phys.Lett. A, 120(1987)87", "J.E. SCHIRBER,D.L. OVERMYER,Jack M. WILLIAMS,H.H. WANG,Lydie VALADE,Patrick CASSOUX", "", "" ] }, { "id": "410", "line_start": 395, "line_end": 395, "sha256": "25fe026c291475c22901a06d9d05d7a79d3dbb9a0195ba6a8b0eb6d1c0689bcb", "values": [ "410", "SYN0700839", "NH4Hg(SCN)4", "alpha-(BEDT-TTF)2NH4Hg(SCN)4", "3", "BEDT-TTF", "", "", "", "", "", "", "1.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC410", "", "", "", "", "anisotyopy (Hc2) = 25 (low temp), = 100 (near Tc).", "OHC410.dat", "", "Anisotropic Hc2, Shubnikov de Haas, and angular dependent magnetoresistance in the organic superconductor a-(BEDT-TTF)2MHg(SCN)4", "1995", "", "Department of Physics, Boston University, Boston, MA", "Synth.Met., 70(1995)839", "J.S.Brooks,S.Uji,H.Aoki,T.Terashima,M.Tokumoto,N.Kinoshita,Y.Tanaka,H.Anzai", "", "" ] }, { "id": "411", "line_start": 396, "line_end": 396, "sha256": "1e91b4462d42e285aa805124bf019711a1b93f64071b915d23c7a0d1817b7df4", "values": [ "411", "J075074606", "AuI2", "(MDT-TSF)(AuI2)0.436", "", "MDT-TSF", "", "", "", "", "", "", "4.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "8.9", "", "", "", "", "", "", "", "", "", "", "", "Thermodynamic Study of an Incommensurate Organic Superconductor (MDT-TSF)(AuI2)0.436", "2006", "", "Department of Chemistry, Graduate School of Science and Engineering, Tokyo Institute of Technology, 2-12-1 Ookayama, Meguro, Tokyo 152-8551", "J.Phys.Soc.Jpn, 75(2006)074606", "Tetsushi ISHIKAWA,Yasuhiro NAKAZAWA,Satoshi YAMASHITA,Masaharu OGUNI,Kazuya SAITO,Kazuo TAKIMIYA,Tetsuo OTSUBO", "", "" ] }, { "id": "412", "line_start": 397, "line_end": 397, "sha256": "8865949869a8ca5dd84eab7f51f35e7a0396a10a00dc4acc637755fa596916ac", "values": [ "412", "L100117002", "ClO4", "(TMTSF)2ClO4", "3", "TMTSF", "", "", "", "", "", "", "1.45", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC412", "", "", "", "", "Hc2, Tc from resistivity measurements", "OHC412.dat", "", "Anomalous In-Plane Anisotropy of the Onset of Superconductivity in (TMTSF)2ClO4", "2008", "", "Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan", "Phys.Rev.Lett., 100(2008)117002", "Shingo Yonezawa,S. Kusaba,Y. Maeno,P. Auban-Senzier,C. Pasquier,K. Bechgaard,D. Jerome", "", "" ] }, { "id": "413", "line_start": 398, "line_end": 398, "sha256": "064a402bb9c0dd4e3265cd7a0c2d80fa5d6691efaf21bed5bb760295c2c94972", "values": [ "413", "J077024714", "PF6", "beta-(meso-DMBEDT-TTF)2PF6", "3", "DMBEDT-TTF", "", "", "", "", "", "", "4.3", "4.3", "", "0.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC413", "", "", "", "", "Tc defined as R(onset).", "OTC413.dat", "", "Infrared and Raman Study of the Charge-Ordered State in the Vicinity of the Superconducting State in the Organic Conductor beta-(meso-DMBEDT-TTF)2PF6", "2008", "", "Institute for Molecular Science and Graduate University for Advanced Studies, Okazaki, Aichi 444-8585", "J.Phys.Soc.Jpn, 77(2008)024714", "Masayuki TANAKA,Kaoru YAMAMOTO,Mikio URUICHI,Takashi YAMAMOTO,Kyuya YAKUSHI,Shinya KIMURA,Hatsumi MORI", "", "" ] }, { "id": "414", "line_start": 399, "line_end": 399, "sha256": "0694facd0d08a0740e3464a6d5680f29862f9daee97f0640e38662130a395120", "values": [ "414", "J077023701", "SbF6", "(TMTTF)2SbF6", "", "TMTTF", "", "", "", "", "", "", "2.3", "2.72", "9", "5.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC414", "", "", "", "", "", "OTC414.dat", "", "Anomalously Wide Superconducting Phase of One-Dimensional Organic Conductor (TMTTF)2SbF6", "2008", "", "Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581", "J.Phys.Soc.Jpn, 77(2008)023701", "Miho ITOI,Chieko ARAKI,Masato HEDO,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "415", "line_start": 400, "line_end": 400, "sha256": "271b52647acab0108243aade50881cb263caa6c076edfa2e711d83cf61fc36af", "values": [ "415", "J077014706", "AuI2", "(MDT-TS)(AuI2)0.441", "3", "MDT-TS", "", "", "", "", "", "", "4.3", "5.14", "1.33", "1.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC415", "", "", "", "", "uniaxial pressure effect of Tc were measured. M-I transitions also measured.", "OTC415.dat", "", "Isotropic Uniaxial Strain Effect on the Incommensurate Organic Superconductor: (MDT-TS)(AuI2)0.441", "2008", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552", "J.Phys.Soc.Jpn, 77(2008)014706", "Yoshimasa BANDO,Tadashi KAWAMOTO,Takehiko MORI,Kazuo TAKIMIYA,Tetsuo OTSUBO", "", "" ] }, { "id": "417", "line_start": 401, "line_end": 401, "sha256": "4c22bb0e596a63e40d7e6e28a3a43357ce921bc56ae9a3ffca0c162e986f61c1", "values": [ "417", "J076123705", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.2", "", "", "0", "", "", "", "", "", "", "", "", "64", "0.43", "", "", "", "", "", "", "", "OHC418", "", "", "", "", "slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence.", "OHC418.dat", "", "Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2", "2007", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 76(2007)123705", "Naoki YONEYAMA,Takahiko SASAKI,Hajime OIZUMI,Norio KOBAYASHI", "", "" ] }, { "id": "418", "line_start": 402, "line_end": 402, "sha256": "e1a2eff40135b8d6a8f8a22c3e14f801225cf893982cafc3b4328d7c47088798", "values": [ "418", "J076123705", "Cu(NCS)2", "kappa-((ET)0.99(MT)0.01)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9", "", "", "0", "", "", "", "", "", "", "", "", "65", "0.445", "", "", "", "", "", "", "", "OHC418", "", "", "", "", "impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence.", "OHC418.dat", "", "Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2", "2007", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 76(2007)123705", "Naoki YONEYAMA,Takahiko SASAKI,Hajime OIZUMI,Norio KOBAYASHI", "", "" ] }, { "id": "419", "line_start": 403, "line_end": 403, "sha256": "6c347bcb83ca47678756778c1ed3fc38a4a47ca8a67f38fcc73ee9e3abe26d85", "values": [ "419", "J076123705", "Cu(NCS)2", "kappa-((ET)0.95(MT)0.05)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "7.9", "", "", "0", "", "", "", "", "", "", "", "", "66", "0.465", "", "", "", "", "", "", "", "OHC418", "", "", "", "", "impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence.", "OHC418.dat", "", "Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2", "2007", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 76(2007)123705", "Naoki YONEYAMA,Takahiko SASAKI,Hajime OIZUMI,Norio KOBAYASHI", "", "" ] }, { "id": "420", "line_start": 404, "line_end": 404, "sha256": "86f761985e986b2b5f6908abddba779139d7325d32ef57348e06ace60c79fbfa", "values": [ "420", "JPS0731290", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.2", "", "", "0", "", "", "", "", "", "", "", "", "", "0.43", "", "", "", "", "", "", "", "OTC421", "", "", "", "", "Tc not depends on cooling rate. [penet] by magnetization.", "OTC421.dat", "", "Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors kappa-(BEDT-TTF)2X (X = Cu(NCS)2 and Cu[N(CN)2]Br)", "2004", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 73(2004)1290", "Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI", "", "" ] }, { "id": "421", "line_start": 405, "line_end": 405, "sha256": "916e13e1b22990b5362cf327f3f27060b20f44adda0e65ef49344313552e8cec", "values": [ "421", "JPS0731290", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.7", "", "", "0", "", "", "", "", "", "", "", "", "", "0.57", "", "", "", "", "", "", "", "", "", "", "", "", "Tc depends on coolong rate (see Fig.). [penet] and Tc in DB shows for coolong rate of 0.2 K/min. [penet] increases with cooling rate. [penet] = 0.69 micron-m for quenched sample (Tc=10.9K).", "", "", "Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors kappa-(BEDT-TTF)2X (X = Cu(NCS)2 and Cu[N(CN)2]Br)", "2004", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577", "J.Phys.Soc.Jpn, 73(2004)1290", "Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI", "", "" ] }, { "id": "422", "line_start": 406, "line_end": 406, "sha256": "edecd9350428d9fa017838b44b6e4426a831c69298b8899c1caecf931eb587ae", "values": [ "422", "P077224506", "AuI2", "(MDT-TS)(AuI2)0.441", "", "MDT-TS", "", "", "", "", "", "", "4.9", "4.9", "1.27", "1.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "50", "", "", "", "", "", "dTc/dP = -6 K/GPa at P=1.27 GPa(Tcmax). SC phase(Tc > 1.5 K) appears for 1.0 < P < 1.8 GPa. ground state = AFI.", "", "", "Antiferromagnetic ordering of the incommensurate organic superconductor (MDT-TS)(AuI2)0.441 with a high spin-flop field", "2008", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan", "Phys.Rev.B, 77(2008)224506", "Tadashi Kawamoto,Yoshimasa Bando,Takehiko Mori,Takako Konoike,Yamaguchi Takahide,Taichi Terashima,Shinya Uji,Kazuo Takimiya,Tetsuo Otsubo", "", "" ] }, { "id": "423", "line_start": 407, "line_end": 407, "sha256": "7cabdbde396ea587ccc203e26dc9ea06e1570e16468010685abd9838277d4cff", "values": [ "423", "PR04912990", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "16.248", "8.44", "13.124", "", "110.3", "", "10.5", "", "", "0", "", "", "", "", "", "", "7", "", "70", "0.768", "125", "", "", "", "", "", "", "", "", "", "", "", "[penet] shows London [penet] calculated from muon-SR result (0.877 micron-m).", "", "", "Magnetic penetration depth and fluxon-line dynamics in the organic superconductor k-[BEDT-TTF]2Cu[NCS]2", "1994", "", "", "Phys.Rev.B, 49(1994)12990", "A.T.Fiory,D.Li.Williams,D.R.Harshman,E.Koster,I.Shinkoda,M.L.Kaplan,R.C.Haddon,T.Pfiz", "organic", "" ] }, { "id": "424", "line_start": 408, "line_end": 408, "sha256": "5a5901c7673091cb90ec32d19b815c71a4368d9ebbfe44b3759cc5ceb2e8beb9", "values": [ "424", "PR05013603", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "8.3", "", "", "0", "", "", "", "", "", "", "", "", "70", "1.4", "", "", "", "", "", "", "", "", "", "", "", "", "surface impedance. For out-of-plane, [penet] = 40 um and [cohere] = 5 A.", "", "", "Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br", "1994", "", "", "Phys.Rev.B.,50(1994) 13603", "G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein", "ORGANIC", "" ] }, { "id": "425", "line_start": 409, "line_end": 409, "sha256": "293c7b9fb4209f15233db5e127f74ca4fb8729d683e730965456d10b50deefd4", "values": [ "425", "PR05013603", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.3", "", "", "0", "", "", "", "", "", "", "", "", "37", "1.5", "", "5", "7", "", "", "", "", "", "", "", "", "", "surface impedance. For out-of-plane, [penet] = 38 um and [cohere] = 6 A.", "", "", "Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br", "1994", "", "", "Phys.Rev.B.,50(1994) 13603", "G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein", "ORGANIC", "" ] }, { "id": "426", "line_start": 410, "line_end": 410, "sha256": "9955797391059a044ead1848091972e69953e924d7c0e84bf9914627e0b4a0de", "values": [ "426", "PR04711595", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "8.3", "", "", "0", "", "", "", "", "", "", "", "", "", "2", "", "", "", "", "", "", "", "", "", "", "", "", "surface impedance.", "", "", "Microwave surface impedance of kappa-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene: Evidence for unconventional superconductivity", "1993", "", "", "Phys.Rev.B, 47(1993)11595", "D.Achkir,M.Poirier,C.Bourbonnais,G.Quirion,C.Lenoir,D.Jerome", "", "" ] }, { "id": "427", "line_start": 411, "line_end": 411, "sha256": "198249640426be9921506a85a0a618f169fc42675ff38678bb74a1427a6f2511", "values": [ "427", "PRB078172506", "SbF6", "beta-(BDA-TTP)2SbF6", "3", "BDA-TTP", "", "", "", "", "", "", "7.32", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC427", "", "", "", "", "P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.", "OTC427.dat", "", "Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression", "2008", "", "Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan", "Phys.Rev.B, 78(2008)172506", "Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi", "", "" ] }, { "id": "428", "line_start": 412, "line_end": 412, "sha256": "be4373483b740c351f7921e4d6f1676d0e970940b5df6c712b537156fcdb301e", "values": [ "428", "PRB078172506", "AsF6", "beta-(BDA-TTP)2AsF6", "3", "BDA-TTP", "", "", "", "", "", "", "6.92", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC428", "", "", "", "", "P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.", "OTC428.dat", "", "Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression", "2008", "", "Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan", "Phys.Rev.B, 78(2008)172506", "Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi", "", "" ] }, { "id": "429", "line_start": 413, "line_end": 413, "sha256": "6af874f6e0f00e7f5d71673d2852cbd3524ad7bbc186d60a7f73a4b770f57810", "values": [ "429", "PRL0792125", "ClO4", "(TMTSF)2ClO4", "3", "TMTSF", "", "", "", "", "", "", "1.2", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "4.6", "3", "", "", "", "", "OTHC429", "", "", "", "", "RRR=440. Tc defined by 0.5Rn. gap obtained by fitting the data of thermal conductivity to BRTmodel. gap has no nodes.", "OTHC429.dat", "", "Thermal Conductivity of Superconducting (TMTSF)2ClO4: Evidence for a Nodeless Gap", "1997", "", "Laboratoire de Physique des Solides (CNRS), Universite Paris-Sud, 91405 Orsay, France", "Phys.Rev.Lett., 79(1997)2125", "Stephane Belin,Kamran Behnia", "", "" ] }, { "id": "430", "line_start": 414, "line_end": 414, "sha256": "9abf0bce9ef33d27d49f7d200f2ffd73c7bc58c23cecb6482238cae5bcf474e4", "values": [ "430", "PRB0428686", "Cu[N(CN)2]Br", "kapa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "11.6", "", "", "0", "", "", "", "", "", "", "", "2.3", "", "", "", "", "", "", "", "", "", "OHC430", "", "", "", "", "Hc2(T) behavior is different between M- and R- definition. Figure shows Hc2 defined as 0.5Rn. The initial (dHc2/dT) is -0.23 and -0.15 T/K for H//ac(donor-plane) and H//b, respectively.", "OHC430.dat", "", "Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor: kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "1990", "", "Argonne National Laboratory, Argonne, Illinois", "Phys.Rev.B, 42(1990)8686", "W.K.Kwok,U.Welp,K.D.Carlson,G.W.Crabtree,K.G.Vandervoort,H.H.Wang,A.M.Kini,J.M.Williams,D.L.Stupka,L.K.Montgomery,J.E.Thompson", "", "" ] }, { "id": "431", "line_start": 415, "line_end": 415, "sha256": "2a86d561ef22bb2dc1f5615c8927716f0a1aaac7bb32ebc1336ec4235c211b7c", "values": [ "431", "PRL0754122", "Cu[N(CN)2]Br", "kapa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "11.6", "", "", "0", "", "", "", "", "", "", "10", "", "60", "", "", "", "", "", "", "", "", "", "", "", "", "", "<13>Cu-NMR. Hc2//b obtained by extraporation assuming Korringa law. For H//ac, this assumption not valid.", "", "", "Superconducting state of kappa-(ET)2Cu{N(CN)2]Br studied by <13>C NMR: Evidence for vortex-core-induced nuclear relaxation and unconventional pairing", "1995", "", "", "Phys.Rev.Lett., 75(1995)4122", "H.Mayaffre,P.Wzietek,D.Jerome,C.Lenoir,P.Batail", "", "" ] }, { "id": "432", "line_start": 416, "line_end": 416, "sha256": "b82debd3bc3bd26a628e7a0e325b46794297aaa8333b5d1c95e5680351f3215a", "values": [ "432", "JPC0163535", "ClO4", "(TMTSF)2ClO4", "3", "TMTSF", "", "", "", "", "", "", "1.221", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "10.5", "213", "", "", "OSP432", "", "", "", "", "(dC) = 21.6 mJ/mol.K. (dC/gamma*Tc) = 1.67. Thermodynamic Hc(0) = 44 Oe. lattice term of SP: beta = 11.5 mJ/mol.K4. SP(H) also measured.", "OSP432.dat", "", "The magnetic field dependence of the specific heat in (TMTSF)2ClO4", "1983", "", "", "J.Phys.C: Solid State Phys., 16(1983)3535", "R Brusetti,P Garoche,K Bechgaard", "", "" ] }, { "id": "433", "line_start": 417, "line_end": 417, "sha256": "1b6339cafa584cae104e369d55ae6bea31aee17e856d80d4a449cb100058a852", "values": [ "433", "PRB080092508", "PF6", "beta-(meso-DMBEDT-TTF)2PF6", "3", "DMBEDT-TTF", "", "", "", "", "", "", "4.6", "4.6", "0.06", "0.06", "", "", "", "-4", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC433", "", "", "", "", "R(min) temperature = 90 K(P=0), 67 K(P=0.6 kbar). (dTc/dP) estimated from average Tc between 0.6 and 5.2 kbar.", "OTC433.dat", "", "Superconductivity competitive with checkerboard-type charge ordering in the organic conductor beta-(meso-DMBEDT-TTF)2PF6", "2009", "", "Institute for Solid State Physics, The University of Tokyo, Kashiwa 277-8581, Japan", "Phys.Rev.B, 80(2009)092508", "Naoki Morinaka,Kazuyuki Takahashi,Ryoma Chiba,Fumiko Yoshikane,Shoichi Niizeki,Masayuki Tanaka,Kyuya Yakushi,Masahito Koeda,Masato Hedo,Tetsuya Fujiwara,Yoshiya Uwatoko,Yutaka Nishio,Kohji Kajita,Hatsumi Mori", "", "" ] }, { "id": "434", "line_start": 418, "line_end": 418, "sha256": "7a29986a76b24cf057c2fb4d588e24585f7c2c73021f77c2c8264d641def5fa5", "values": [ "434", "JPCS150052224", "Cu(NCS)2", "kappa-[(BEDT-TTF)1-x(BMDT-TTF)x]2Cu(NCS)2", "3", "BEDT-TTF", "", "", "", "", "", "", "9.26", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC434", "", "", "", "", "samples with (BMDT-TTF) impurity as a scattering center. scattering effect on Tc were measured.", "OTC434.dat", "", "Disorder effect on superconductivity in organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2009", "", "Institute for Materials Research, Tohoku University, 980-8577 Sendai, Japan", "J.Phys.: Conf.Series, 150(2009)052224", "T. Sasaki,H. Oizumi,N. Yoneyama,N. Kobayashi", "", "" ] }, { "id": "435", "line_start": 419, "line_end": 419, "sha256": "1e3ab72cf089060dd6eee6d512d9dfe2e610d5961853475b81062af3ef5fa5ae", "values": [ "435", "EPL08527009", "[Au(mnt)]2", "(Per)2[Au(mnt)]2", "3", "Per", "", "", "", "", "", "", "0.313", "0.313", "0.53", "0.53", "", "", "", "", "", "", "0.0494", "", "", "", "", "", "", "", "", "", "", "OHC435", "", "", "", "", "(Per) = perylene. Hc2(0) = 49.4 mT at P = 5.3 kbar. Hc2 defined as R=0.9Rn. T = 12 K.", "OHC435.dat", "", "Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2]", "2009", "", "Physics/NHMFL Florida State University - Tallahassee, FL 32310, USA", "Europhys.Lett., 85(2009)27009", "D. Graf,J. S. Brooks,M. Almeida,J. C. Dias,S. Uji,T. Terashima,M. Kimata", "", "" ] }, { "id": "436", "line_start": 420, "line_end": 420, "sha256": "3fdcf7103b3199f53a5e3522f3e33e67c30e6f59f296a32f81b4245112edffc0", "values": [ "436", "JPCS150052093", "IBrCl", "beta'-(BEDT-TTF)2IBrCl", "3", "BEDT-TTF", "", "", "", "", "", "", "8.5", "8.5", "8.6", "8.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC only for 8.6 =< P =<8.8 GPa. Tc(on) = 8.5 K, Tc(zero) = 4.0 K at 8.6 GPa (broad transition)", "", "", "Superconductivity induced by extremely high pressures in organic Mott-insulator beta'-(BEDTTTF)2IBrCl", "2009", "", "National High Magnetic Field Laboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA", "J.Phys.: Conf.Series, 150(2009)052093", "M Kano,K Uchiyama,H Taniguchi,M Hedo,K Matsubayashi,Y Uwatoko", "", "" ] }, { "id": "437", "line_start": 421, "line_end": 421, "sha256": "81bd41f4a3ac969fd34591f3184c909f126284339965e29aa89a3e1323d6e588", "values": [ "437", "PHB4043246", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "2.27", "", "4.48", "4.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC437", "", "", "", "", "Hc2 defined as Tc(on). Hc2 for H//a, H//b', H//c* were measured at P = 4.48 GPa.", "", "", "Anisotropy of the upper critical field in ultrahigh-pressure-induced superconductor (TMTTF)2PF6", "2009", "", "National HigMagnetiFielLaboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA", "Physica B, 404(2009)3246", "Mika Kano,Hatsumi Mori,Yoshiya Uwatoko,Stan Tozer", "", "" ] }, { "id": "438", "line_start": 422, "line_end": 422, "sha256": "cc6920ed4f168010247c54ce01484fd851bf1c7e266a281bea0d73584b9871eb", "values": [ "438", "PHB405S262", "I3", "beta-(BEDT-TTF)2I3", "", "BEDT-TTF", "", "", "", "", "", "", "1.5", "9", "0.4", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC438", "", "", "", "", "donor stack (along c-axis). FIG shows uniaxial-P effect of Tc. 8K-phase stabilized by embedding crystal into epoxy.", "OTC438.dat", "", "Superconductivityof beta-type salts under uniaxial compression", "2010", "", "Department of Applied Physics, Nagoya University, Japan", "Physica B, 405(2010)S262", "Hiroshi Ito,Tetsuo Ishihara,Masafumi Niwa,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Hideki Yamochi,Gunzi Saito", "", "" ] }, { "id": "439", "line_start": 423, "line_end": 423, "sha256": "f0611ad69826b85776e6556377fe574298bf794c5d1357a8b6e765e5cc05d408", "values": [ "439", "PHB405S291", "Br", "(TMTTF)2Br", "3", "TMTTF", "", "", "", "", "", "", "0.8", "", "", "3.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "uniaxial pressure (//a-axis) induces SC at 3.7 GPa. crystals grown by electrochemical method.", "", "", "First observation of superconductivity by uniaxial strain in (TMTTF)2X-salt", "2010", "", "Graduate School of Science, Osaka City University, Japan", "Physica B, 405(2010)S291", "Keiichi Yokogawa,Harukazu Yoshino,Toshikazu Nakamura,James S.Brooks,Keizo Murata", "", "" ] }, { "id": "440", "line_start": 424, "line_end": 424, "sha256": "81ad0866dbe103ae6d2a43cca4261172e2e515b29799c9664673dad02f039ae9", "values": [ "440", "JTL0460188", "Hg0.89Br8", "(BEDT-TTF)4Hg0.89Br8", "3", "BEDT-TTF", "", "", "", "", "", "", "4.3", "", "", "0", "", "", "", "", "", "", "", "10", "343", "", "", "", "", "", "", "", "", "OHC440", "", "", "", "", "comprised of two incommensulate monoclinic lattices. For H//c, (dHc2/dT) = 1.8 T/K, and cohere(//c) = 17 A.", "OHC440.dat", "", "Superconductivity of (ET)4Hg2.89Br8 at atmospheric pressure and Tc = 4.3 K and the critical-field anisotropy", "1987", "", "", "JETP Lett., 46(1987)188", "R.N.Lyubovskaya,E.I.Zhilyaeva,S.I.Pesotskii,R.B.Lyubovskii,L.O.Atovmyan,O.A.D'yachenko,T.G.Takhirov", "", "" ] }, { "id": "441", "line_start": 425, "line_end": 425, "sha256": "710a6037e94510da8505b88341ff86ea34d3d76d4d939d848d0da374c7e37452", "values": [ "441", "PRB081020512", "ICl2", "beta'-(BEDT-TTF)2ICl2", "3", "BEDT-TTF", "", "", "", "", "", "", "14.2", "14.2", "8.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "22", "OTC441", "", "", "", "", "<13>C NMR measured. AFM-phase has the moment of 0.47 myu-B/dimer at 0.6 GPa, 26 K. FIG shows Tn(P).", "OTC441.dat", "", "Antiferromagnetic phase in beta-(BEDT-TTF)2ICl2 under pressure as seen via <13>C NMR", "2010", "", "Department of Quantum and Condensed Matter Physics, Graduate School of Science, Hokkaido University, Kita-ku, Sapporo, Hokkaido 060-0810, Japan", "Phys.Rev.B, 81(2010)020512", "Yoshihiro Eto,Atsushi Kawamoto", "", "" ] }, { "id": "442", "line_start": 426, "line_end": 426, "sha256": "cf82c1a343d787b5af58ea072af12867c7e2bff0af102735a76faee516b36041", "values": [ "442", "PRB081100509", "PF6", "(TMTSF)2PF6", "3", "TMTSF", "", "", "", "", "", "", "1.24", "1.24", "0.9", "0.66", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC442", "", "", "", "", "Tc depends on P-direction. P = 0.66, 0.78, 0.86 GPa for uniaxial pressure of c-, b-, a-axis direction, respectively. T goes to 0 K at 0.94 GPa, independent of P-direction.", "OTC442.dat", "", "Domain walls at the spin-density-wave endpoint of the organic superconductor (TMTSF)2PF6 under pressure", "2010", "", "Laboratoire de Physique des Solides, UMR 8502-CNRS, Universite Paris-Sud, Orsay F-91405, France", "Phys.Rev.B, 81(2010)100509", "N. Kang,B. Salameh,P. Auban-Senzier,D. Jerome,C. R. Pasquier,S. Brazovskii", "", "" ] }, { "id": "443", "line_start": 427, "line_end": 427, "sha256": "49f8d7b213b164018ddc247557d07e99ff33468b83792b8c687d73d6ad42de0b", "values": [ "443", "JPS080054706", "[Au(CN)4](THF)", "kappa-(DMEDO-TSeF)2[Au(CN)4](THF)", "3", "DMEDO-TSeF", "", "", "", "", "", "", "2.2", "", "", "0", "", "", "", "", "", "", "", "", "510", "", "", "", "", "", "", "", "", "OHC443", "", "", "", "", "Tc defined as R=0.5Rn. cohere(//ab) =510 A. cohere(//c) = 3.5 A. [cohere] estimated from (dHc2/dT) which values not given clearly. Anisotropy(cohere) = 150", "OHC443.dat", "", "Two-Dimensional Superconducting Properties of the Organic Superconductor kappa-(DMEDO-TSeF)2[Au(CN)4](THF) with Domain Structures", "2011", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, Meguro, Tokyo 152-8552, Japan", "J.Phys.Soc.Jpn, 80(2011)054706", "Tadashi KAWAMOTO,Takehiko MORI,Takashi SHIRAHATA,Tatsuro IMAKUBO", "", "" ] }, { "id": "444", "line_start": 428, "line_end": 428, "sha256": "2477ebd353d9256d89c0764d4f2f7cc68e99d38bc68bf006070d787fbc0503ad", "values": [ "444", "PRB081024519", "AuBr2", "beta''-(BEDT-TTF)2AuBr2", "", "BEDT-TTF", "", "", "", "", "", "", "1.1", "1.1", "1", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC444", "", "", "", "", "c-axis(in a-c plane)-induced SC. T = 6.5 K. uniaxial pressure applied using epoxy method.", "OTC444.dat", "", "Interplay of charge-density waves and superconductivity in the organic conductor beta''-(BEDT-TTF)2AuBr2", "2010", "", "Department of Basic Science, University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan", "Phys.Rev.B, 81(2010)024519", "Ryusuke Kondo,Momoka Higa,Seiichi Kagoshima,Noriaki Hanasaki,Yoshio Nogami,Hiroyuki Nishikawa", "", "" ] }, { "id": "445", "line_start": 429, "line_end": 429, "sha256": "10b2860e5962f670b29ab592b6a76a3ccb5396d6aaf2fc7d0aaee73c303058ca", "values": [ "445", "ACS12412430", "[(H3O)Ga(C2O4)3](C5H5N)", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3](C5H5N)", "", "BEDT-TTF", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "0.4", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC. R(T) has a broad maximum at about 50 K. I //conducting plane.", "", "", "Effect of Included Guest Molecules on the Normal State Conductivity and Superconductivity of beta''-(ET)4[(H3O)Ga(C2O4)3]:G (G = Pyridine, Nitrobenzene )", "2002", "", "DaVy Faraday Research Laboratory, The Royal Institution of Great Britain", "J.Am.Chem.Soc, 124(2002)12430", "Hiroki Akutsu,Akane Akutsu-Sato,Scott S. Turner,Delphine Le Pevelen,Peter Day,Vladimir Laukhin,Anne-Katrin Klehe,John Singleton,Derek A. Tocher,Michael R. Probert,Judith A. K. Howard", "", "" ] }, { "id": "446", "line_start": 430, "line_end": 430, "sha256": "8eb684b482a315b101d9cf1c8f3f54166b936eeef850d9dae6246217a8d34666", "values": [ "446", "ACS12412430", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "7.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC volume = 31 % at 1.8 K.. R measured for I //conducting plane.", "", "", "Effect of Included Guest Molecules on the Normal State Conductivity and Superconductivity of beta''-(ET)4[(H3O)Ga(C2O4)3]:G (G = Pyridine, Nitrobenzene )", "2002", "", "DaVy Faraday Research Laboratory, The Royal Institution of Great Britain", "J.Am.Chem.Soc, 124(2002)12430", "Hiroki Akutsu,Akane Akutsu-Sato,Scott S. Turner,Delphine Le Pevelen,Peter Day,Vladimir Laukhin,Anne-Katrin Klehe,John Singleton,Derek A. Tocher,Michael R. Probert,Judith A. K. Howard", "", "" ] }, { "id": "447", "line_start": 431, "line_end": 431, "sha256": "73881ca50d9d2f415597d050218ef9556ea4881191aa2e0522003e0c16b07c0f", "values": [ "447", "PRB081092508", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "2", "", "", "", "2.5", "", "", "", "", "", "energy gap measured by infrared reflectance. (2d/kTc) = 8.", "", "", "Low-temperature far-infrared absorption in the antiferromagnetic organic superconductor kappa-(BETS)2FeBr4", "2010", "", "Department of Physics, Brock University, St. Catharines, Ontario, Canada L2S 3A1", "Phys.Rev.B, 81(2010)092508", "N. Hossein Khah,G. V. Sudhakar Rao,M. Reedyk,H. Fujiwara,H. Kobayashi,T. Nakamura,K. Yakushi,M. A. Tanatar", "", "" ] }, { "id": "448", "line_start": 432, "line_end": 432, "sha256": "0c1943b487036ee8b6b86f18e70a1102464fb807167449e5c4f5cc08bc85b9c5", "values": [ "448", "PRB083014505", "I3", "(DMET)2I3", "", "DMET", "", "", "", "", "", "", "0.58", "", "", "0", "", "", "", "", "", "", "0.79", "", "271", "", "", "", "", "", "", "", "", "OHC448", "", "", "", "", "Hc2(0) = 0.79, 0.186, 0.019 t for H//x-, y-, z-axis. Cohere(i) = 271, 64, 6.5 A for I = x, y, z , using Hc2(0) = (fai)/2(pai)*q*q.", "OHC448.dat", "", "Upper critical field of the molecular organic superconductor (DMET)2I3", "2011", "", "Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467, USA", "Phys.Rev.B, 83(2011)014505", "Pashupati Dhakal,Harukazu Yoshino,Jeong Il Oh,Koichi Kikuchi,Michael J. Naughton", "", "" ] }, { "id": "449", "line_start": 433, "line_end": 433, "sha256": "e36ab27a35424cc0c976955de66e97dd52c28cd24a893e870d87739675032f3c", "values": [ "449", "PRB082155123", "Mn[N(CN)2]3", "kappa-(BETS)2Mn[N(CN)2]3", "", "BETS", "19.4723", "8.4135", "11.9608", "90", "92.315", "90", "5.75", "5.75", "0.05", "0.04", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC449", "", "", "", "", "density = 2.371 g/cm3. quasi static pressure.", "OTC449.dat", "", "Temperature-pressure phase diagram and electronic properties of the organic metal kappa-(BETS)2Mn[N(CN)2]3", "2011", "", "1Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, Garching, Germany", "Phys.Rev.B, 82(2010)155123", "V. N. Zverev,M. V. Kartsovnik,W. Biberacher,S. S. Khasanov,R. P. Shibaeva,L. Ouahab,L. Toupet,N. D. Kushch,E. B. Yagubskii,E. 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Tc(zero) = 0.5 K.", "", "", "Scanning tunnelling spectroscopy study of paramagnetic superconducting beta''-ET4[(H3O)Fe(C2O4)3]:C6H5Br crystals", "2010", "", "CNR-SPIN, Complesso Universitario di Monte S Angelo, Via Cinthia, 80126 Napoli, Italy", "J.Phys.:Condens.Matter, 22(2010)175701", "A Gambardella,M Salluzzo,R Di Capua,M Affronte,CGimenez-Saiz,C JGomez-Garcia,E Coronado,R Vaglio", "", "" ] }, { "id": "451", "line_start": 435, "line_end": 435, "sha256": "97fa798be2818fb47b1b3a76686bfdd05ecbbfff914cb0581d6c460d9f7bbcaf", "values": [ "451", "EPJ0780023", "PF6", "(TMTSF)2PF6", "", "TMTSF", "", "", "", "", "", "", "1.22", "1.22", "0.92", "0.65", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH451", "", "", "", "", "Tc defined as Tc(on) for J//ab.", "OPH451.dat", "", "Linear-T scattering and pairing from antiferromagnetic fluctuations in the (TMTSF)2X organic superconductors", "2010", "", "Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, J1K 2R1, Canada", "Eur.Phys.J.B, 78(2010)23", "N. Doiron-Leyraud,S. Rene de Cotret,A. Sedeki,C. Bourbonnais,L. Taillefer,P. Auban-Senzier,D. Jerome,K. Bechgaard", "", "" ] }, { "id": "452", "line_start": 436, "line_end": 436, "sha256": "5eb5149d548e4d52e6f4553f9aefb172364b35334a65f5d8f98f8171fa8435b0", "values": [ "452", "EPJ0780023", "ClO4", "(TMTSF)2ClO4", "", "TMTSF", "", "", "", "", "", "", "1.45", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH452", "", "", "", "", "Tc defined as Tc(on) for J//ab. Tc= 0 K at P=1.03 GPa.", "OPH452.dat", "", "Linear-T scattering and pairing from antiferromagnetic fluctuations in the (TMTSF)2X organic superconductors", "2010", "", "Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, J1K 2R1, Canada", "Eur.Phys.J.B, 78(2010)23", "N. Doiron-Leyraud,S. Rene de Cotret,A. Sedeki,C. Bourbonnais,L. Taillefer,P. Auban-Senzier,D. Jerome,K. 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Kang,B. Salameh,P. Auban-Senzier,D. Jerome,C. R. Pasquier,S. Brazovskii", "", "" ] }, { "id": "455", "line_start": 439, "line_end": 439, "sha256": "ac6d87a4e7c73c9df02b791b2bb87e12703094ee6de79c8163e2a733fd6c1f81", "values": [ "455", "JPS080074702", "Cu2(CN)3", "kappa-(BEDT-TTF)2Cu2(CN)3", "3", "BEDT-TTF", "", "", "", "", "", "", "4", "7.3", "0.3", "0", "", "", "", "7", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC455", "", "", "", "", "Mott transition T increases with increasing P for all uniaxial pressure. 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FIG shows X-ray irradiation effect of Tc ( Tc vs irradiation time of X-ray)", "OTC458.dat", "", "Suppression of Superconductivity by Nonmagnetic Disorder in Organic Superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2011", "", "Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 80(2011)104703", "Takahiko SASAKI,Hajime OIZUMI,Yuki HONDA,Naoki YONEYAMA,Norio KOBAYASHI", "", "" ] }, { "id": "459", "line_start": 443, "line_end": 443, "sha256": "8bf49c9852b515a03f1562ae6d86a67b66adccca210adb37ac5f58f0675da8f6", "values": [ "459", "JPCM022175701", "[(H3O)Fe(C2O4)3]:PhBr", "beta''-(ET)4[(H3O)Fe(C2O4)3]:PhBr", "", "BEDT-TTF", "", "", "", "", "", "", "4", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "17.1", "1", "", "", "", "", "", "", "", "", "", "Tc(zero) = 0.5 K. 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Naughton", "", "" ] }, { "id": "461", "line_start": 445, "line_end": 445, "sha256": "a28c15a6a588156727723b9042886b05649245a90fc8983160650abd938474e6", "values": [ "461", "PRB083024504", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.3", "", "", "0", "", "", "", "", "", "", "", "", "", "0.47", "", "", "", "", "", "", "", "", "", "", "", "", "For H < 3 mT , in-plane penetration depth measured by muon-SR .", "", "", "Superconductivity and fluctuating magnetism in quasi-two-dimensional kappa-(BEDT-TTF)2Cu[N(CN)2]Br probed with implanted muons", "2011", "", "Oxford University Department of Physics, Clarendon Laboratory, Parks Road, Oxford, OX1 3PU, United Kingdom", "Phys.Rev.B, 83(2011)024504", "T. Lancaster,S. J. Blundell,F. L. Pratt,J. A. 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T decreases from 20 K(P=0) to 5K (P=3.7 GPa) for uniaxial (a-axis) stress.", "", "", "First observation of superconductivity by uniaxial strain in (TMTTF)2X-salt", "2010", "", "Graduate School of Science, Osaka City University, Japan", "Physica B, 405(2010)S291", "Keiichi Yokogawa,Harukazu Yoshino,Toshikazu Nakamura,James S.Brooks,Keizo Murata", "", "" ] }, { "id": "464", "line_start": 448, "line_end": 448, "sha256": "0f953c4fb0b7b560de95451901eca87e3f21cd2f2d254e1ee81c65b68ac644b1", "values": [ "464", "SYN0700899", "RbHg(SCN)", "kappa-(ET)2RbHg(SCN)4", "", "BEDT-TTF", "", "", "", "", "", "", "0.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "There appears SC-like resistivity decrease both in in-plane and out-of-plane resistivity.", "", "", "Superconductivity in alpha-(BEDT-TTF)2MHg(SCN)4 (M=K, Rb, Tl, NH4)", "1995", "", "Department of Physics, kyoto University, Kyoto 606-01, Japan", "Synth.Met., 70(1995)899", "H.Ito,M.V.Kartsovink,H.Ishimoto,K.Kono,H.Mori,N.D.Kushch,G.Saito,T.Ishiguro,S.Tanaka", "", "" ] }, { "id": "465", "line_start": 449, "line_end": 449, "sha256": "aa5f3f9822a80d60af4945cbfb347746537998b7f6bff30acc0c792696763982", "values": [ "465", "SYN0700899", "TlHg(SCN)4", "kappa-(ET)2TlHg(SCN)4", "", "BEDT-TTF", "", "", "", "", "", "", "0.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Superconductivity in alpha-(BEDT-TTF)2MHg(SCN)4 (M=K, Rb, Tl, NH4)", "1995", "", "Department of Physics, kyoto University, Kyoto 606-01, Japan", "Synth.Met., 70(1995)899", "H.Ito,M.V.Kartsovink,H.Ishimoto,K.Kono,H.Mori,N.D.Kushch,G.Saito,T.Ishiguro,S.Tanaka", "", "" ] }, { "id": "466", "line_start": 450, "line_end": 450, "sha256": "e098ea15a33321460f4330593829109e4ad22e1ddf5da0797302bba9ff38b305", "values": [ "466", "PHC3510261", "I3", "beta-(BEDT-TTF)2I3", "", "BEDT-TTF", "", "", "", "", "", "", "8", "", "", "0", "", "-0.6", "C", 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SC-volume fraction = 39.5 %. Space-group : P2<1>.", "", "", "Superconductivity in A1.5phenanthrene (A=Sr,Ba)", "2011", "", "Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China", "Phys.Rev.B, 84(2011)214523", "X. F. Wang,Y. J. Yan,Z. Gui,R. H. Liu,J. J. Ying,X. G. Luo,X. H. Chen", "", "" ] }, { "id": "494", "line_start": 478, "line_end": 478, "sha256": "da4b9c7876750e9a30037e7f9bd65d36b1ad5288b0c80800afb50b55ab0525b9", "values": [ "494", "PRB084214523", "", "Ba1.5-phenanthrene", "", "phenanthrene", "8.479", "6.177", "9.502", "", "97.49", "", "5.4", "", "", "0", "", "", "", "1.24", "", "72", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ba-doped phenanthrene. SC-volume fraction = 65.4 %. Hc1 at 2 K. Space-group : P2<1>", "", "", "Superconductivity in A1.5phenanthrene (A=Sr,Ba)", "2011", "", "Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China", "Phys.Rev.B, 84(2011)214523", "X. F. Wang,Y. J. Yan,Z. Gui,R. H. Liu,J. J. Ying,X. G. Luo,X. H. Chen", "", "" ] }, { "id": "495", "line_start": 479, "line_end": 479, "sha256": "6a1f8984eaea972914e68043f974dce54387c705bb663470dc5dbf5ff009d4ca", "values": [ "495", "NAT4640076", "K2.9", "K2.9Picene", "", "Picene", "8.707", "5.912", "12.97", "", "92.77", "", "7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "alkali metal doping prepared by ANN(440K, 9.0 days). shielding fraction = 0.1 %.", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "496", "line_start": 480, "line_end": 480, "sha256": "8388b31426151fd9f88fe3ae75f139ff6cc6a706f358a91654b08b39070c216a", "values": [ "496", "NAT4640076", "K3.3", "K3.3Picene", "", "Picene", "", "", "", "", "", "", "18", "", "", "0", "", "", "", "", "", "38", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "alkali metal doping prepared by ANN(440K, 11 days). shielding fraction = 1.2 %.", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "497", "line_start": 481, "line_end": 481, "sha256": "694c5482f7a11be46c61f1953d157b0ba43b7e9e98eca8b9d8e381ecfead1202", "values": [ "497", "NAT4640076", "Rb3.1", "Rb3.1Picene", "", "Picene", "", "", "", "", "", "", "6.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "alkali metal doping prepared by ANN(570K, 6.7 days). shielding fraction = 10 %.", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "498", "line_start": 482, "line_end": 482, "sha256": "1e42c228ff1f9482c9a7c4c3ceb2ee19132a6fdfb4be9258bd81798cd4f8c656", "values": [ "498", "NATCOM0020507", "K3", "K3-phenanthrene", "", "phenanthrene", "8.43", "6.134", "9.417", "", "98.18", "", "4.95", "", "", "0", "", "", "", "1.17", "", "175", "", "", "", "", "", "", "", "", "", "3.634", "", "OTC498", "OHC498", "", "", "", "SC-volume = 5.3%. Hc1(2.5K) = 175 Oe. SC only for x=3 (investigated for 2.5 < x < 3.5 , nominal value x in Kx-phenanthrene). Hc2 defined as SUS(onset).", "OTC498.dat", "OHC498.dat", "Superconductivity at 5 K in alkali-metal-doped phenanthrene", "2011", "", "Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science ant Technology of China, Hefei, Anhui 230026, China", "Nature Commun., 2(2011)507", "X.F.Wang,R.H.Liu,Z.Gui,Y.L.Xie,Y.J.Yan,J.J.Ying,X.G.Luo,X.H.Chen", "", "" ] }, { "id": "499", "line_start": 483, "line_end": 483, "sha256": "bccb5be0361e87753ccf6b6386ac49959b033b6a15ad315e2e196c4b35798e1a", "values": [ "499", "NATCOM0020507", "Rb3", "Rb3-phenanthrene", "", "phenanthrene", "8.45", "6.139", "9.442", "", "97.99", "", "4.75", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "3.99", "", "", "", "", "", "", "SC-volume = 6.7%.", "", "", "Superconductivity at 5 K in alkali-metal-doped phenanthrene", "2011", "", "Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science ant Technology of China, Hefei, Anhui 230026, China", "Nature Commun., 2(2011)507", "X.F.Wang,R.H.Liu,Z.Gui,Y.L.Xie,Y.J.Yan,J.J.Ying,X.G.Luo,X.H.Chen", "", "" ] }, { "id": "500", "line_start": 484, "line_end": 484, "sha256": "772252de051041ec71db9de85e91a5962619537e5e33dbbdb64fa58990ba174d", "values": [ "500", "JPCM0086005", "Cl2/2H2O", "(BEDT-TTF)3Cl2/2H2O", "2", "BEDT-TTF", "", "", "", "", "", "", "3.6", "3.6", "1.13", "1.02", "", "", "", "", "", "", "", "", "150", "", "", "", "", "", "", "", "", "OTC500", "", "", "", "", "T = 25 K at P=0. Tc < 0.7 K at P=1.45 GPa. cohere = 150A (P=1.13 GPa) and 170A (P=1.25 GPa).", "", "", "A study of the magnetoresistance of the charge-transfer salt (BEDT-TTF)3Cl2/2H2O at hydrostatic pressures of up to 20 kbar: evidence for a charge-density-wave ground state and the observation of pressure-induced superconductivity", "1996", "", "Department of Physics, University of Oxford, Clarendon Laboratory, Oxford,UK", "J.Phys.:Condens.Matter, 8(1996)6005", "W.Lubczynski,S.V.Demishev,J.Singleton,J.M.Caulfield,L.du Croo de Jongh,C.J.Kepert,S.J.Blundell,W.Hayes,M.Kurmoo,P.Day", "", "" ] }, { "id": "501", "line_start": 485, "line_end": 485, "sha256": "6e0471f67e72fde302672f9734deb24dbd2c886f0b8e0a93a418cb786a51ee7d", "values": [ "501", "PRB081092508", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "8", "", "", "", "", "2.5", "", "", "", "", "", "Anisotropic energy gap measured by FIR measurements. thermal reflectance along a- and c- axis were measured.", "", "", "Low-temperature far-infrared absorption in the antiferromagnetic organic superconductor kappa-(BETS)2FeBr4", "2010", "", "Department of Physics, Brock University, St. Catharines, Ontario, Canada L2S 3A1", "Phys.Rev.B, 81(2010)092508", "N. Hossein Khah,G. V. Sudhakar Rao,M. Reedyk,H. Fujiwara,H. Kobayashi,T. Nakamura,K. Yakushi,M. A. Tanatar", "", "" ] }, { "id": "600", "line_start": 486, "line_end": 486, "sha256": "246c645510ac29df44d54b466c6b40389b668ef59be039d1424afdf7387f3357", "values": [ "600", "PRB085214520", "Ba1.5", "Ba1.5-phenanthrene", "2", "phenanthrene", "", "", "", "", "", "", "4.7", "", "", "0", "", "", "", "", "", "", "0.7", "0.208", "217", "", "", "3.9", "14", "17", "255", "", "", "OSP600", "OHC600", "", "", "", "crystal grown from melt(Ba+phenanthrene), annealed. gap defined fron SP. Hc2 from WHH-clean limit. gamma(normal volume) = 3.03 mJ/mol.K2.", "OSP600.dat", "OHC600.dat", "Bulk superconductivity and fully gapped superconducting state in Ba-doped phenanthrene", "2012", "", "Quantum-Phase Electronics Center (QPEC) and Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan", "Phys.Rev.B, 85(2012)214520", "Yuichi Kasahara,Yuki Takeuchi,Yoshihiro Iwasa", "", "" ] }, { "id": "601", "line_start": 487, "line_end": 487, "sha256": "aab54b9cc71682489f4d42a6b0e80ff91c0765070cab3d5910fc617e3c7a21be", "values": [ "601", "PRB085180511", "Ba1.5", "Ba1.5-phenanthrene", "2", "phenanthrene", "", "", "", "", "", "", "4.9", "", "", "0", "", "", "", "", "", "", "1.2", "0.333", "", "", "", "3.9", "14", "17.8", "260", "", "", "OHC601", "", "", "", "", "pellet heat(230C,8d). sample is single-gap s-wavw SC. (dC/Tc) = 31 mJ/mol.K2. (dC/gamma(n)*Tc) = 2.03. gamma(DB) = gamma(n) + gamma(0): 17.8=15.3+2.5 mJ/mol.K2", "OHC601.dat", "", "s-wave superconductivity in barium-doped phenanthrene as revealed by specific-heat measurements", "2012", "", "Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China", "Phys.Rev.B, 85(2012)180511", "Jianjun Ying,Xiangfeng Wang,Yajun Yan,Ziji Xiang,Xigang Luo,Zhe Sun,Xianhui Chen", "", "" ] }, { "id": "602", "line_start": 488, "line_end": 488, "sha256": "8f25cd501b2b262c1f2fd2a292e0f0ae5140c3b89110b3fd1c1ab507e951b172", "values": [ "602", "PRB085140502", "ClO4", "(TMTSF)2ClO4", "2", "TMTSF", "", "", "", "", "", "", "1.3", "", "", "0", "", "", "", "", "", "", "", "8.1", "", "", "", "", "", "", "", "", "", "OHC602-1", "OHC602-2", "", "", "", "grown by electro crystallization. mean free pass = 1.6 um. C(H) measured for various angle of a-b plane. (dHc2/dT) = 2.3 and 0.11 T/K for H//b', and H//c* axis .", "OHC602-1.dat", "OHC602-2.dat", "Nodal superconducting order parameter and thermodynamic phase diagram of (TMTSF)2ClO4", "2012", "", "Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan", "Phys.Rev.B, 85(2012)140502", "Shingo Yonezawa,Yoshiteru Maeno,Klaus Bechgaard,Denis Jerome", "", "" ] }, { "id": "603", "line_start": 489, "line_end": 489, "sha256": "bf6722b6f80587b5d9508d64e7c64d3e9e8786e00a80d51fc3d2be9e045ad345", "values": [ "603", "JPS081024716", "PF6", "(TMTTF)2PF6", "", "TMTTF", "", "", "", "", "", "", "2.27", "2.3", "4.58", "4.18", "", "", "", "", "", "", "", "0.864", "264", "", "", "", "", "", "", "", "", "OHC603", "", "", "", "", "P-induced SC. nearly hydrostatic P. SC data for P = 4.48 GPa.. (dHc2/dT)b' = 0.738, (dHc2/dT)c* = 0.246 T/K. cohere(b') = 223, cohere(c*) = 75.1 A. Hc2 measured for a, b', c* direction.", "OHC603.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "604", "line_start": 490, "line_end": 490, "sha256": "038eb4014f0a4a953b258517ec5420b6538cb88eed5ec05f8d1c462fd6791353", "values": [ "604", "JPS081024716", "PF6", "(TMTTF)2PF6", "", "TMTTF", "", "", "", "", "", "", "1.89", "2.3", "4.58", "4.18", "", "", "", "", "", "", "", "0.773", "338", "", "", "", "", "", "", "", "", "OHC604", "", "", "", "", "P-induced SC. nearly hydrostatic P. SC data for P = 5.10 GPa.. (dHc2/dT)b' = 0.630, (dHc2/dT)c* = 0.187 T/K. cohere(b') = 276, cohere(c*) = 81.8 A. Hc2 measured for a, b', c* direction.", "OHC604.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "605", "line_start": 491, "line_end": 491, "sha256": "474ded84a6450e1e4ecc93117366019ab6a9e263084932bd4f9173fcd6f3a059", "values": [ "605", "JPS081024716", "PF6", "(TMTTF)2PF6", "", "TMTTF", "", "", "", "", "", "", "1.51", "2.3", "4.58", "4.18", "", "", "", "", "", "", "0.47", "0.457", "499", "", "", "", "", "", "", "", "", "OHC605", "", "", "", "", "P-induced SC. nearly hydrostatic P. SC data for P = 5.64 GPa.. (dHc2/dT)b' = 0.465, (dHc2/dT)c* = 0.086 T/K. cohere(b') = 507, cohere(c*) = 94.0 A. Hc2 measured for a, b', c* direction.", "OHC605.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "606", "line_start": 492, "line_end": 492, "sha256": "cbe4cc137f884574c95319dd6afe8e7f054878a0ea7792c7c91336e9a18f4cdd", "values": [ "606", "JPS081024716", "PF6", "(TMTTF)2PF6", "", "TMTTF", "", "", "", "", "", "", "2.3", "2.3", "4.58", "4.18", "", "", "", "", "", "", "1.36", "0.86", "", "", "", "", "", "", "", "", "", "OHC606", "OPH606", "", "", "", "P-induced SC. nearly hydrostatic P. SC data for P = 4.58 GPa.. SP: spin Peierls, CL: charged localized in OPH606(Fig)", "OHC606.dat", "OPH606.dat", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "610", "line_start": 493, "line_end": 493, "sha256": "cba130c8ff7844e8d8fedfc99ea240a68a59e6990f7f5c39c99774bce43beec4", "values": [ "610", "PRB085220506", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "10.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC610", "", "", "", "", "grown by electrochemical method. Hc2 measured by torque and resistivity. There exists \"fluctuating SC states, FSC\".", "OHC610.dat", "", "Fluctuating superconductivity in the strongly correlated two-dimensional organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 in an in-plane magnetic field", "2012", "", "National Institute for Materials Science, Ibaraki 305-0003, Japan", "Phys.Rev.B, 85(2012)220506", "Satoshi Tsuchiya,Jun-ichi Yamada,Satoshi Tanda,Koichi Ichimura,Taichi Terashima,Nobuyuki Kurita,Kota Kodama,Shinya Uji", "", "" ] }, { "id": "611", "line_start": 494, "line_end": 494, "sha256": "dc0596492c9099e1532007e1baad032b3d890912c69f8b7d3adc690097bb18f3", "values": [ "611", "PRB087060505", "K3.1", "KxPicene", "", "Picene", "", "", "", "", "", "", "6.7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "mixture(Kx,Picene) - sealed in pyrex tube - annealed(473K,10days). R(300) = 0.42 Ohm.cm, R(10) = 100 Ohm.cm", "", "", "Observation of zero resistivity in K-doped picene", "2013", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Phys.Rev.B, 87(2013)060505", "Kazuya Teranishi,Xuexia He,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Ritsuko Eguchi,Yasuhiro Takabayashi,Takashi Kambe,Yoshihiro Kubozono", "", "" ] }, { "id": "612", "line_start": 495, "line_end": 495, "sha256": "f942c049c5e79631d97cd404187694fa83ad389b19e226827d6c96f6ba536d11", "values": [ "612", "PRB087060505", "K3.5", "KxPicene", "", "Picene", "8.579", "5.843", "13.13", "", "94.37", "", "10.9", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "mixture(Kx,Picene) - sealed in pyrex tube - annealed(473K,10days). R(300) = 0.28 Ohm.cm.", "", "", "Observation of zero resistivity in K-doped picene", "2013", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Phys.Rev.B, 87(2013)060505", "Kazuya Teranishi,Xuexia He,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Ritsuko Eguchi,Yasuhiro Takabayashi,Takashi Kambe,Yoshihiro Kubozono", "", "" ] }, { "id": "615", "line_start": 496, "line_end": 496, "sha256": "c0dca29e758f3852bf42426b6550682b10bb872c0aa286a9056f12d3bd276915", "values": [ "615", "JPC024345701", "La1", "La1-phenanthrene", "", "phenanthrene", "8.481", "6.187", "9.512", "", "97.95", "", "6.1", "", "", "", "", "", "", "1.53", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC615", "OHC615", "", "", "", "Space group: P2<1>. SC volume fraction=46.1% at 2.5K. (dTc/dP)/Tc = 0.25 GPa(-1). Effective magnetic moment= 0.34 Myu-B/mol", "OTC615.dat", "OHC615.dat", "Enhanced superconductivity by rare-earth metal doping in phenanthrene", "2012", "", "Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China", "J.Phys.: Condens.Matter, 24(2012)345701", "X F Wang,X G Luo,J J Ying,Z J Xiang,S L Zhang,R R Zhang,Y H Zhang,Y J Yan,A F Wang,P Cheng,G J Ye,X H Chen", "", "" ] }, { "id": "616", "line_start": 497, "line_end": 497, "sha256": "cde41b502ef6fd7156b86f330685f71afbbf5d2e0fce0714e15d779a5adc9cd1", "values": [ "616", "JPC024345701", "Sm1", "Sm1-phenanthrene", "", "phenanthrene", "8.475", "6.18", "9.505", "", "98.1", "", "6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "15", "", "", "", "", "", "Space group: P2<1>. SC volume fraction=49.8% at 2.5K. Effective magnetic moment= 0.64 Myu-B/mol", "", "", "Enhanced superconductivity by rare-earth metal doping in phenanthrene", "2012", "", "Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China", "J.Phys.: Condens.Matter, 24(2012)345701", "X F Wang,X G Luo,J J Ying,Z J Xiang,S L Zhang,R R Zhang,Y H Zhang,Y J Yan,A F Wang,P Cheng,G J Ye,X H Chen", "", "" ] }, { "id": "617", "line_start": 498, "line_end": 498, "sha256": "5447d6d009f1baf74ac0c49fc19cdedecc557ced7d4a6fbb750dd54f96ebf452", "values": [ "617", "JPS081024716", "PF6", "(TMTTF)2PF6", "", "TMTTF", "", "", "", "", "", "", "2.1", "2.27", "4.58", "4.2", "", "", "", "", "", "", "4.5", "", "", "", "", "", "", "", "", "", "", "OTC617", "OHC617", "", "", "", "Tc = 2.30, 1.79, 1.51 K and Hc2(0)//a = 4.5 T(linear fitting), 1.27, 0.50 T for P=4.58, 5.23, 5.64 GPa, respectively.", "OTC617.dat", "OHC617.dat", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "618", "line_start": 499, "line_end": 499, "sha256": "115d74cc6031239f893f215d8c76de16ad12a4b79bf12d7abcc9b6b4420d4a3a", "values": [ "618", "JPS081024716", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "2.27", "", "", "", "", "", "", "", "", "", "", "0.864", "264", "", "", "", "", "", "", "", "", "OHC618", "", "", "", "", "SC properties at 4.48 GPa. DB values of (dHc2/dT) and cohere for H//a. (dHc2/dT)=0.738, 0.246 T/K and cohere=223, 75.1 A for H//b' and c*, respectively.", "OHC618.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "619", "line_start": 500, "line_end": 500, "sha256": "bd13d009f5e69f42754b8df256a2346f5cc88f0637d9e8bde76d6e0161c51a96", "values": [ "619", "JPS081024716", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "1.89", "", "", "", "", "", "", "", "", "", "", "0.773", "338", "", "", "", "", "", "", "", "", "OHC619", "", "", "", "", "SC properties at 5.10 GPa. DB values of (dHc2/dT) and cohere for H//a. (dHc2/dT)=0.630, 0.187 T/K and cohere=276, 81.8 A for H//b' and c*, respectively.", "OHC619.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "620", "line_start": 501, "line_end": 501, "sha256": "e990a39af31ffd4507f72f21440b82fe0e6f4d6ac3ba068fbf0f4ab6b9c103dd", "values": [ "620", "JPS081024716", "PF6", "(TMTTF)2PF6", "3", "TMTTF", "", "", "", "", "", "", "1.51", "", "", "", "", "", "", "", "", "", "", "0.457", "499", "", "", "", "", "", "", "", "", "OHC620", "", "", "", "", "SC properties at 5.64 GPa. DB values of (dHc2/dT) and cohere for H//a. (dHc2/dT)=0.465, 0.086 T/K and cohere=507, 94.0 A for H//b' and c*, respectively.", "OHC620.dat", "", "Anisotropy of Upper Critical Field in a One-Dimensional Organic System, (TMTTF)2PF6 under High Pressure", "2012", "", "Institute for Material Research, Tohoku University, Sendai 980-8577, Japan", "J.Phys.Soc.Jpn, 81(2012)024716", "Mika KANO,Hatsumi MORI,Kazuyuki MATSUBAYASHI,Miho ITOI,Masato HEDO,Timothy P. MURPHY,Stanley W. TOZER,Yoshiya UWATOKO,Toshikazu NAKAMURA", "", "" ] }, { "id": "621", "line_start": 502, "line_end": 502, "sha256": "1bc48f00acbfb4a77bf8e9a2f0e02047f20dd6aff0ccdac7811f0e52a347c2dd", "values": [ "621", "PHB4071715", "TTF", "TTF[Ni(dmit)2]2", "", "Ni(dmit)2", "", "", "", "", "", "", "1.71", "", "", "0.7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTHP621", "", "", "", "", "Tc(on), Tc(mid), Tc(zero) are 1.71, 1.21, 1.07, respectively. Thermopower(THP) were measured for various P. Figure shows for P=0.8 GPa. THP300 = -20 uV/K at 300 K.", "OTHP621.dat", "", "Thermoelectric power of TTF[Ni(dmit)2]2", "2012", "", "Laboratoire de Physique des Solides, UMR8502-CNRS, Universite Paris-Sud, Bat. 510, Orsay F-91405, France", "Physica B, 407(2012)1715", "Wafa Kaddour,PascaleAuban-Senzier,ClaudePasquier,LydieValade", "", "" ] }, { "id": "622", "line_start": 503, "line_end": 503, "sha256": "08bc40a192bb042c654f1421999657fba7c3286d9e9a2dcbfcdc319845da8c44", "values": [ "622", "PHB4071919", "KHg(SCN)4", "alpha-(BEDT-TTF)2KHg(SCN)4", "", "BEDT-TTF", "", "", "", "", "", "", "0.11", "", "", "0.25", "", "", "", "", "", "", "0.007", "12", "2200", "", "", "", "", "", "", "", "", "OHC622", "", "", "", "", "For T=>0.9, (dHc2/dT)//layer = 12 T/K. [cohere]/n/layer = 11 A. Hc2/n/layer = 7 mT. then [cohere]// = 2200 A. Anisotropy(cohere) = 200.", "OHC622.dat", "", "Magnetic field effects on the charge-density-wave and superconducting states in pressurized alpha-(BEDT-TTF)2KHg(SCN)4", "2012", "", "Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, 85748 Garching, Germany", "Physica B, 407(2012)1919", "M.V. Kartsovnik,W.Biberacher,D.Andres,S.Jakob,M.Kunz,K. Neumaier,H.Muller,N.D.Kushch", "", "" ] }, { "id": "623", "line_start": 504, "line_end": 504, "sha256": "eb58d6c28afb7cf3074fb1d858919cdda431141067742d04190e6a1575012c19", "values": [ "623", "PRB086214507", "K3.3", "K3.3-Picene", "", "Picene", "", "", "", "", "", "", "7.1", "", "", "", "", "", "", "-0.3", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC623", "", "", "", "", "7 K phase. Tc = Tc(mid)", "OTC623.dat", "", "Synthesis and physical properties of metal-doped picene solids", "2012", "", "Department of Physics, Okayama University, Okayama 700-8530, Japan", "Phys.Rev.B, 86(2012)214507", "Takashi Kambe,Xuexia He,Yosuke Takahashi,Yusuke Yamanari,Kazuya Teranishi,Hiroki Mitamura,Seiji Shibasaki,Keitaro Tomita,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kato,Akihiko Fujiwara,Toshikaze Kariyado,Hideo Aoki,Yoshihiro Kubozono", "", "" ] }, { "id": "624", "line_start": 505, "line_end": 505, "sha256": "24bd385e4cb2a6ec7e239e3faf67b1a45f632a84c212ba142e92830914d87760", "values": [ "624", "PRB086214507", "K3.3", "K3.3-Picene", "", "Picene", "8.571", "6.27", "14.001", "", "91.68", "", "15", "", "", "", "", "", "", "12.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC624", "", "", "", "", "18 K phase. Tc = Tc(on). volume = 752 A3", "OTC624.dat", "", "Synthesis and physical properties of metal-doped picene solids", "2012", "", "Department of Physics, Okayama University, Okayama 700-8530, Japan", "Phys.Rev.B, 86(2012)214507", "Takashi Kambe,Xuexia He,Yosuke Takahashi,Yusuke Yamanari,Kazuya Teranishi,Hiroki Mitamura,Seiji Shibasaki,Keitaro Tomita,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kato,Akihiko Fujiwara,Toshikaze Kariyado,Hideo Aoki,Yoshihiro Kubozono", "", "" ] }, { "id": "625", "line_start": 506, "line_end": 506, "sha256": "69cb480f91c59feee03a43b6db35efebf73d872c9f2e498a1a6221791eb2060f", "values": [ "625", "PRL099187002", "Cu(NCS)2", "k-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.1", "", "", "", "", "", "", "", "", "", "130", "20", "", "", "", "", "", "26", "200", "", "", "OHC625", "", "", "", "", "Hc2(0)//plane calculated from (dHc2/dT) at Tc using WHH. (dC) = 0.58 J/mol.K. (dC/gamma*Tc) = 2.5.", "OHC625.dat", "", "Calorimetric Evidence for a Fulde-Ferrell-Larkin-Ovchinnikov Superconducting State in the Layered Organic Superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2007", "", "Department of Condensed Matter Physics, University of Geneva, CH-1211 Geneva 4, Switzerland", "Phys.Rev.Lett., 99(2007)187002", "R. Lortz,Y. Wang,A. Demuer,P. H. M. Bottger,B. Bergk,G. Zwicknagl,Y. Nakazawa,J. Wosnitza", "", "" ] }, { "id": "626", "line_start": 507, "line_end": 507, "sha256": "b1df150ee0f3bffb5074e779331142068d43667fea86a2586d4f29349e5480b0", "values": [ "626", "JPC0086005", "Cl2/H2O", "(BEDT-TTF)3Cl2/H2O", "3", "BEDT-TTF", "", "", "", "", "", "", "2.9", "3.6", "1.13", "1.02", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC626", "", "", "", "", "Tc defined as R=0.95Rn. M-I transition at 150 K. CDW observed below T", "", "", "A study of the magnetoresistance of the charge-transfer salt (BEDT-TTF)3Cl2/H2O at hydrostatic pressures of up to 20 kbar: evidence for a charge-density-wave ground state and the observation of pressure-induced superconductivity", "1996", "", "", "J.Phys.Condens Matter, 8(1996)6005", "W Lubczynski,S V Demishev,J Singleton,J M Caulfield,L du Croo de Jongh,C J Kepert,S J Blunde,W Hayes,M Kurmoo,P.Day", "", "" ] }, { "id": "627", "line_start": 508, "line_end": 508, "sha256": "36308ee30d126df594b8f3323f96497b75e0efa033d6c7b0d2d9449421e5a663", "values": [ "627", "JPS081023705", "Ag(CF3)4(THE)", "kappa/alpha1'-(BEDT-TTF)2Ag(CF3)4(THE)", "3", "BEDT-TTF", "", "", "", "", "", "", "9.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "4-layered structure composed of kappa- and alpha--type donor sheets. Tc measured by torque method", "", "", "Tc of 11K Identified for the Third Polymorph of the (BEDT-TTF)2Ag(CF3)4(TCE) Organic Superconductor", "2012", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, Meguro, Tokyo 152-8552, Japan", "J.Phys.Soc.Jpn, 81(2012)023705", "Tadashi KAWAMOTO,Takehiko MORI,Akiko NAKAO,Youichi MURAKAMI,John A. SCHLUETER", "", "" ] }, { "id": "628", "line_start": 509, "line_end": 509, "sha256": "55582f431807c7086caa2657727945a6a4c7f31601a719e8eee015ad5324142e", "values": [ "628", "JPS081023705", "Ag(CF3)4(THE)", "kappa/alpha2'-(BEDT-TTF)2Ag(CF3)4(THE)", "3", "BEDT-TTF", "", "", "", "", "", "", "11.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "4-layered structure composed of kappa- and alpha--type donor sheets. Tc measured by torque method", "", "", "Tc of 11K Identified for the Third Polymorph of the (BEDT-TTF)2Ag(CF3)4(TCE) Organic Superconductor", "2012", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, Meguro, Tokyo 152-8552, Japan", "J.Phys.Soc.Jpn, 81(2012)023705", "Tadashi KAWAMOTO,Takehiko MORI,Akiko NAKAO,Youichi MURAKAMI,John A. SCHLUETER", "", "" ] }, { "id": "629", "line_start": 510, "line_end": 510, "sha256": "141252bd0ba72b1356db8521317defe7495a94e847071764b0b950a5347212af", "values": [ "629", "JPS082083701", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "", "", "", "", "", "", "6.7", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc(H=4T) = 3.5 K, Tc(H=7T) = 2.8 K for H//b-axis. FM,AM abrupt increases below T = 12K (charge instability. <13>C-NMR measured.", "", "", "<13>C NMR Study of Superconductivity near Charge Instability Realized beta''-(BEDT-TTF)4[H3O)Ga(C2O4)3]:C6H5NO2", "2013", "", "Department of Physics, Graduate School of Science, Hokkaido University, Sapporo, Japan", "J.Phys.Soc.Jpn, 82(2013)083701", "Yoshihiko Ihara,Harumi Seki,Atsushi Kawamoto", "", "" ] }, { "id": "630", "line_start": 511, "line_end": 511, "sha256": "ff4367aeeda838e3ee05dc4ffd8a88f5d8bf7ec0c13b5f2f2c2e561f90575b7c", "values": [ "630", "PRB083064506", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.32", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC630", "", "", "", "", "Hc2(T) and H measured by torque measurements. H anomaly at H = 21 T appears from angular dependence of torque.", "OHC630.dat", "", "Magnetic torque evidence for the Fulde-Ferrell-Larkin-Ovchinnikov state in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2011", "", "Hochfeld-Magnetlabor Dresden (HLD), Forschungszentrum Dresden-Rossendorf, D-01314 Dresden, Germany", "Phys.Rev.B, 83(2011)064506", "B. Bergk,A. Demuer,I. Sheikin,Y. Wang,J. Wosnitza,Y. Nakazawa,R. Lortz", "", "" ] }, { "id": "631", "line_start": 512, "line_end": 512, "sha256": "85c57abedeb149c34fd8154f449bc8a8dd53a957c1d21bb6c0094f3e560d2659", "values": [ "631", "JPS081023705", "Ag(CH3)4(TCE)", "kappa-alpha'(2)-(BEDT-TTF)2Ag(CH3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "11", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "4 layered structure composed of kappa- and alpha'- type donor sheets", "", "", "Tc of 11K Identified for the Third Polymorph of the (BEDT-TTF)2Ag(CF3)4(TCE) Organic Superconductor", "2012", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, Meguro, Tokyo 152-8552, Japan", "J.Phys.Soc.Jpn, 81(2012)023705", "Tadashi KAWAMOTO,Takehiko MORI,Akiko NAKAO,Youichi MURAKAMI,John A. SCHLUETER", "", "" ] }, { "id": "632", "line_start": 513, "line_end": 513, "sha256": "3b9998d75ed0dbdcac2ff7c825de130f26025840ceb38a6c1d7e8d4ebcff14f4", "values": [ "632", "JPS081023705", "Ag(CH3)4(TCE)", "kappa-alpha'(1)-(BEDT-TTF)2Ag(CH3)4(TCE)", "", "BEDT-TTF", "", "", "", "", "", "", "9.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "2 layered structure composed of kappa- and alpha'- type donor sheets", "", "", "Tc of 11K Identified for the Third Polymorph of the (BEDT-TTF)2Ag(CF3)4(TCE) Organic Superconductor", "2012", "", "Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, Meguro, Tokyo 152-8552, Japan", "J.Phys.Soc.Jpn, 81(2012)023705", "Tadashi KAWAMOTO,Takehiko MORI,Akiko NAKAO,Youichi MURAKAMI,John A. SCHLUETER", "", "" ] }, { "id": "633", "line_start": 514, "line_end": 514, "sha256": "566529bcb6ad9cbab19db49e8f9e22ee67dc6c0db9f8364215dc671da40bd521", "values": [ "633", "JPS082064711", "Cu[(N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[(N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "12", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC633", "", "", "", "", "Fluctuating SC phase (FSC-phase) appears using magnetic torque measurements", "OHC633.dat", "", "Fluctuating Superconductivity in the Strongly Correlated Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "2013", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "J.Phys.Soc,Jpn, 82(2013)064711", "Satoshi TSUCHIYA,Jun-ichi YAMADA,Taichi TERASHIMA,Nobuyuki KURITA,Kota KODAMA,Kaori SUGII,Shinya UJI", "", "" ] }, { "id": "634", "line_start": 515, "line_end": 515, "sha256": "4a94d669e7073ff17505253b570bb18c2e8c426ec7e2486e2ce7c6c14836dae2", "values": [ "634", "PCCP01316476", "K3", "K3-picene", "", "Picene", "", "", "", "", "", "", "7", "", "", "0", "", "", "", "", "", "30", "", "", "180", "0.095", "", "", "", "", "", "", "", "OHC634", "", "", "", "", "Tc= 7K phase. Hc measured by SUS.", "OHC634.dat", "", "Metal-intercalated aromatic hydrocarbons: a new class of carbon-based superconductors", "2011", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan.", "Phys.Chem.Chem.Phys., 13(2011)16476", "Yoshihiro Kubozono,Hiroki Mitamura,Xuesong Lee,Xuexia He,Yusuke Yamanari,Yosuke Takahashi,Yuta Suzuki,Yumiko Kaji,Ritsuko Eguchi,Koki Akaike,Takashi Kambe,Hideki Okamoto,Akihiko Fujiwara,Takashi Kato,Taichi Kosugi,Hideo Aoki", "", "" ] }, { "id": "635", "line_start": 516, "line_end": 516, "sha256": "ad0c9389b7059b9131ec89f7a74bd106f78dea234033b32e01412a1219cca579", "values": [ "635", "PCCP01316476", "K3", "K3-picene", "", "Picene", "", "", "", "", "", "", "18", "", "", "0", "", "", "", "", "", "", "", "", "180", "0.077", "", "", "", "", "", "", "", "OHC635", "", "", "", "", "Tc=18 K phase. Hc measured by SUS.", "OHC635.dat", "", "Metal-intercalated aromatic hydrocarbons: a new class of carbon-based superconductors", "2011", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan.", "Phys.Chem.Chem.Phys., 13(2011)16476", "Yoshihiro Kubozono,Hiroki Mitamura,Xuesong Lee,Xuexia He,Yusuke Yamanari,Yosuke Takahashi,Yuta Suzuki,Yumiko Kaji,Ritsuko Eguchi,Koki Akaike,Takashi Kambe,Hideki Okamoto,Akihiko Fujiwara,Takashi Kato,Taichi Kosugi,Hideo Aoki", "", "" ] }, { "id": "636", "line_start": 517, "line_end": 517, "sha256": "06449649d92fa39e35e629a28de528d600771cb00c41b3f2948e360a0a747863", "values": [ "636", "PCCP01316476", "Rb3", "Rb3-picene", "", "Picene", "", "", "", "", "", "", "7", "", "", "0", "", "", "", "", "", "8", "", "", "570", "0.13", "", "", "", "", "", "", "", "OHC636", "", "", "", "", "Hc measured by SUS.", "OHC636.dat", "", "Metal-intercalated aromatic hydrocarbons: a new class of carbon-based superconductors", "2011", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan.", "Phys.Chem.Chem.Phys., 13(2011)16476", "Yoshihiro Kubozono,Hiroki Mitamura,Xuesong Lee,Xuexia He,Yusuke Yamanari,Yosuke Takahashi,Yuta Suzuki,Yumiko Kaji,Ritsuko Eguchi,Koki Akaike,Takashi Kambe,Hideki Okamoto,Akihiko Fujiwara,Takashi Kato,Taichi Kosugi,Hideo Aoki", "", "" ] }, { "id": "637", "line_start": 518, "line_end": 518, "sha256": "de82cf5a6dec88d8ea6c301edf4737f6a02eadc3c5db75eab315cef558f133bf", "values": [ "637", "PCCP01316476", "Ca1.5", "Ca1.5-picene", "", "Picene", "", "", "", "", "", "", "7", "", "", "0", "", "", "", "", "", "15", "", "", "570", "0.1", "", "", "", "", "", "", "", "OHC637", "", "", "", "", "Hc measured by SUS. SC volume fraction = 1.25 % at 2K", "OHC637.dat", "", "Metal-intercalated aromatic hydrocarbons: a new class of carbon-based superconductors", "2011", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan.", "Phys.Chem.Chem.Phys., 13(2011)16476", "Yoshihiro Kubozono,Hiroki Mitamura,Xuesong Lee,Xuexia He,Yusuke Yamanari,Yosuke Takahashi,Yuta Suzuki,Yumiko Kaji,Ritsuko Eguchi,Koki Akaike,Takashi Kambe,Hideki Okamoto,Akihiko Fujiwara,Takashi Kato,Taichi Kosugi,Hideo Aoki", "", "" ] }, { "id": "638", "line_start": 519, "line_end": 519, "sha256": "d5efba4063f9f92d942179a87b79583dd54da08de7abf5d2880236fb87f0221f", "values": [ "638", "PCCP01316476", "K3", "K3-coronene", "", "coronene", "16.117", "4.7039", "10.099", "", "111.025", "", "15", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC-volume fraction = 0.5 %. Tc = 3.5, 7, 11, 15 K are observed for samples, where (K:coronene = 3:1) annealed (573K, in vac(1E-5 Torr)", "", "", "Metal-intercalated aromatic hydrocarbons: a new class of carbon-based superconductors", "2011", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan.", "Phys.Chem.Chem.Phys., 13(2011)16476", "Yoshihiro Kubozono,Hiroki Mitamura,Xuesong Lee,Xuexia He,Yusuke Yamanari,Yosuke Takahashi,Yuta Suzuki,Yumiko Kaji,Ritsuko Eguchi,Koki Akaike,Takashi Kambe,Hideki Okamoto,Akihiko Fujiwara,Takashi Kato,Taichi Kosugi,Hideo Aoki", "", "" ] }, { "id": "639", "line_start": 520, "line_end": 520, "sha256": "ce4dea72498df84c419416f4c8e47614ba5a3116c833baec6de8a575e015592c", "values": [ "639", "PRB0465822", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "DEDT-TTF", "", "", "", "", "", "", "11.4", "", "", "0", "", "", "", "", "", "1.9", "", "", "", "0.78", "", "3.88", "", "", "", "", "", "", "", "", "", "", "[penet] from dM/d(lnH). GL-parameter, Hc1 estimated using clean limit formulas.", "", "", "Magnetic penetration depth of kappa-(BEDT-TTF)2Cu[N(CN)2]Br, determined from the reversible magnetization", "1992", "", "Institute for Materials Research, Tohoku University, Sendai 980, Japan", "Phys.Rev.B, 46(1992)5822", "M.Lang,N.Toyota,T.Sasaki,H.Sato", "", "" ] }, { "id": "640", "line_start": 521, "line_end": 521, "sha256": "70d1fa6708f6a90faeb545aea3afee7acab263b80c948a9824704e23c84dd13f", "values": [ "640", "JPS084054601", "AuI2", "(DMET)2AuI2", "", "DMET", "", "", "", "", "", "", "0.5", "", "", "0.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTP640", "OTHC640", "", "", "", "T = 16 K. Thermal conductivity k has two independent Debye terms with Debye-T = 79 and 340 K. K(200K) = 4 W/K.m. There appears max value at 70K in k(T)", "OTP640.dat", "OTHC640.dat", "Thermal Conductivity of Molecular Crystal with Various Types of Chemical Bonding: Quasi-One-Dimensional Organic Superconductor (DMET)2AuI2", "2015", "", "Graduate School of Science, Osaka City University, Osaka 558-8585, Japan", "J.Phys.Soc.Jpn, 84(2015)054601", "Yoshiki Iwasaki,Harukazu Yoshino,Natsuki Kuroda,Koichi Kikuchi,Keizo Murata", "", "" ] }, { "id": "641", "line_start": 522, "line_end": 522, "sha256": "c6ca3ea93aae8e1aa4bba62f02cdfea939f0801012bfefb4eb5712ffa833f739", "values": [ "641", "JPS084063704", "GaCl4", "ramda-(BEDT-STF)2GaCl4", "", "BEDT-TSF", "16.207", "18.293", "6.579", "98.488", "97.04", "112.33", "5", "5.75", "1.35", "1.22", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC641", "", "", "", "", "samples prepared by standard electrochemical method. R(300)/R(6K) = 40 at 1.60 GPa for #A and = 3 at P=1.90 GPa for #B. T is metal-insulator transition", "OTC641.dat", "", "Superconducting Phase in ramda-(BEDT-STF)2GaCl4 at High Pressures", "2015", "", "Department of Physics, Hokkaido University, Sapporo 060-0810, Japan", "J.Phys.Soc.Jpn, 84(2015)063704", "Takaaki Minamidate,Yuki Oka,Hironori Shindo,Toshitaka Yamazaki,Noriaki Matsunaga,Kazushige Nomura,Atsushi Kawamoto", "", "" ] }, { "id": "642", "line_start": 523, "line_end": 523, "sha256": "7f1145416597d125b3e4ceaf4ef95bbc66ce05ea6b826cdfcdd50a0c91770379", "values": [ "642", "JPS084064713", "Cu[N(CN)2]Br", "kappa-(d-[3:3]BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "11.9", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "7.8", "1", "", "", "", "", "", "", "", "", "", "Energy gap measured by STS(tunneling spectroscopy) at 1.2 K on the a-c plane. gap d(0) = 4.0 meV", "", "", "Tunneling Spectroscopy in Organic Superconductor kappa-(BEDT-TTF-d[3,3])2Cu[N(CN)2]Br", "2015", "", "Department of Physics, Hokkaido University, Sapporo 060-0810, Japan", "J.Phys.Soc.Jpn, 84(2015)064713", "Yuki Oka,Hiroyoshi Nobukane,Noriaki Matsunaga,Kazushige Nomura,Kazuhiro Katono,Koichi Ichimura,Atsushi Kawamoto", "", "" ] }, { "id": "643", "line_start": 524, "line_end": 524, "sha256": "3dda349ed6f94d1a16e6a0698e0fd5e67525e663c38749cdeb54f55878efe165", "values": [ "643", "JPS084094709", "SF5CH2CF2SO3", "beta''-(BEDT)2SF5CH2CF2SO3", "", "BEDT-TTF", "", "", "", "", "", "", "5.1", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC643-1", "OHC643-2", "", "", "", "Anisotropy and angular dependence of Hc2 were measured. Sample A (Tc=5.1K), B (Tc= 5.2 K)", "OHC643-1.dat", "OHC643-2.dat", "In-Plane Anisotropy of Upper Critical Field and Flux-Flow Resistivity in Layered Organic Superconductor beta''-(ET)2SF5CH2CF2SO3", "2015", "", "Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan", "J.Phys.Soc.Jpn, 84(2015)094709", "Syuma Yasuzuka,Shinya Uji,Taichi Terashima,Kaori Sugii,Takayuki Isono,Yoritsugu Iida,John A. Schlueter", "", "" ] }, { "id": "644", "line_start": 525, "line_end": 525, "sha256": "f1ddc4f6bca87114b1d3458db5610491c67c5d6a2ac7aaa177b2d080ba3216d9", "values": [ "644", "JPS084104709", "GaCl4", "ramda-(BETS)2GaCl4", "3", "BETS", "", "", "", "", "", "", "6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC644", "", "", "", "", "RRR = 300. R(T) max at 80 K. R-peak appears below Tc(onset) and depends on angle between ac-plane and b*. H//c (defined as R(onset) ) measured .", "OHC644.dat", "", "Vortex Dynamics and Diamagnetic Torque Signals in Two Dimensional Organic Superconductor ramda-(BETS)2GaCl4", "2015", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "J.Phys.Soc.Jpn, 84(2015)104709", "Shinya Uji,Kouta Kodama,Kaori Sugii1,Taichi Terashima,Takahide Yamaguchi,Nobuyuki Kurita,Satoshi Tsuchiya,Takako Konoike,Motoi Kimata,Akiko Kobayashi,Biao Zhou,Hayao Kobayashi", "", "" ] }, { "id": "645", "line_start": 526, "line_end": 526, "sha256": "dbc914cb31a06fe4dff4887dc36d7a19c9f810022fff686b653d40e17b8dabab", "values": [ "645", "PHC5140199", "K3", "K3-picene", "", "picene", "", "", "", "", "", "", "14", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC-volume = 3.9% at 2K.", "", "", "Superconductivity in aromatic hydrocarbons", "2015", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Physica C, 514(2015)199", "Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu", "", "" ] }, { "id": "646", "line_start": 527, "line_end": 527, "sha256": "d1c10c15aea7f6749b87e0e52a90835f34ed9291c76efc39523ea73a1a5081fa", "values": [ "646", "PHC5140199", "K3", "K3-[7]phenacene", "", "phenacene", "", "", "", "", "", "", "11", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC-volume = 0.1% at 2K.", "", "", "Superconductivity in aromatic hydrocarbons", "2015", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Physica C, 514(2015)199", "Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu", "", "" ] }, { "id": "647", "line_start": 528, "line_end": 528, "sha256": "c51c37b3a354604513349bed67c03091ee690418323963cb66b24babbc1c681e", "values": [ "647", "PHC5140199", "Sr1.5", "Sr1.5-phenanthrene", "", "phenanthrene", "", "", "", "", "", "", "6", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "SC-volume = 4% at 2K. Tc(SUS) = 5.3 K.", "", "", "Superconductivity in aromatic hydrocarbons", "2015", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Physica C, 514(2015)199", "Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu", "", "" ] }, { "id": "648", "line_start": 529, "line_end": 529, "sha256": "614970b136dbe269aba19311b984fceed66879b5c282026a9d7ca91efc888f8e", "values": [ "648", "PHC5140199", "Kx", "Kx-DBP", "", "DBP", "", "", "", "", "", "", "30", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Sample has two-phases: Tc1 = 30K, Tc2 = 7K. , corresponding to different x in Kx-DBP. DBP = dibenzopentacene", "", "", "Superconductivity in aromatic hydrocarbons", "2015", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Physica C, 514(2015)199", "Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu", "", "" ] }, { "id": "650", "line_start": 530, "line_end": 530, "sha256": "7eee12f98c70e189f50b8e28952e322b08c4d972c584c84206141a619d538e06", "values": [ "650", "JPS085014601", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "10.251", "20.05", "35.19", "", "92.326", "", "7.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "130", "", "", "OSP650", "", "", "", "", "There exist the kink at 90 K in C(T) and lattice parameters due to charge ordering. Debye-T = 130 K for T < 50 K fittong.", "OSP650.dat", "", "High-Temperature Charge and Structure Anomalies in (beta)''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]/C6H5NO2", "2016", "", "Department of Condensed Matter Physics, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan", "J.Phys.Soc.Jpn, 85(2016)014601", "Yoshihiko Ihara,Yosuke Futami,Atsushi Kawamoto", "", "" ] }, { "id": "651", "line_start": 531, "line_end": 531, "sha256": "f3a0c194638930330bdd951f46a74200c80ead9f2746c552d77ade6e207eb0ac", "values": [ "651", "JPS085023601", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "8.4", "OPH651", "", "", "", "", "H-induced SC. (dC) = C - C(lattice) measured under H//c. Tn obtained from the peak of (dC) for 3 samples for H < 11T", "OPH651.dat", "", "Effective Field Study of Canted Antiferromagnetic Insulating Phase in Magnetic Organic Conductor ramda-(BETS)2FeCl4 through Specific Heat Measurement", "2016", "", "Department of Physics, Toho University, Funabashi, Chiba 274-8510, Japan", "J.Phys.Soc.Jpn, 85(2016)023601", "Kazuo Shimada,Naoya Tajima,Koji Kajita,Yutaka Nishio", "", "" ] }, { "id": "652", "line_start": 532, "line_end": 532, "sha256": "6c9acb78cfa620cd6e0dfe13b6934837c88dc249507eeca0ccab68538f8a35ce", "values": [ "652", "JPS085043705", "GaCl4", "ramda-(BETS)2GaCl4", "", "BETS", "", "", "", "", "", "", "4.8", "", "", "0", "", "", "", "", "", "", "3.5", "", "", "", "", "", "", "20.6", "", "", "", "", "", "", "", "", "C = a*T + b*T^3 + c*T^5 + Einstein term(E1, E2): b = 18.2 mJ/mol.K4, c = 0.024 mJ/mol.K6, E1 = 30.6 K, E2 = 46.7 K from data fitting.", "", "", "Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4", "2016", "", "Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan", "J.Phys.Soc.Jpn, 85(2016)043705", "Shusaku Imajo,Naoki Kanda,Satoshi Yamashita,Hiroki Akutsu,Yasuhiro Nakazawa,Hiroya Kumagai,Takuya Kobayashi,Atsushi Kawamoto", "", "" ] }, { "id": "655", "line_start": 533, "line_end": 533, "sha256": "f9fe2d33f57d11a82dfe573f5b36cd1564444480d2a1901357daa67b9acdff1a", "values": [ "655", "PRB094020503", "CF3SO3", "kappa-(BEDT-TTF)2CF3SO3", "3", "BEDT-TTF", "", "", "", "", "", "", "4.7", "4.8", "1.3", "1.1", "", "", "", "", "", "", "", "", "370", "", "", "", "", "", "", "", "", "OHC655", "OTC655", "", "", "", "SC-data at P = 1.45 GPa. Hc2 defined as midpoint. Hc2 depend on current direction", "OHC655.dat", "OTC655.dat", "Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice", "2016", "", "Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan", "Phys.Rev.B, 94(2016)020503", "Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito", "", "" ] }, { "id": "656", "line_start": 534, "line_end": 534, "sha256": "93a09a2f5fa4bad10fc9581ac35099ed68e0af46d59be758294ccffa302ca501", "values": [ "656", "PRB094020503", "CF3SO3", "kappa-(BEDT-TTF)2CF3SO3", "3", "BEDT-TTF", "", "", "", "", "", "", "4.98", "4.98", "1.9", "1.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTC656", "", "", "", "", "Tc for c-axis pressure (strain)", "OTC656.dat", "", "Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice", "2016", "", "Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan", "Phys.Rev.B, 94(2016)020503", "Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito", "", "" ] }, { "id": "660", "line_start": 535, "line_end": 535, "sha256": "2fef7368c7639cafd649b58ec8694f0fd327ad4e78da084bc8317feed40141d1", "values": [ "660", "PRB095165133", "(Fe,Ga)Cl4", "lambda-(BETS)2Fe0.63Ga0.37Cl4", "", "BETS", "", "", "", "", "", "", "5.05", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "2.9", "OPH660", "", "", "", "", "Fig shows anti-ferro-insulator (AFI), SC, PM phases , measured by T-sweep, R-sweep resistance and torque method. kink- and dip-temperature in R(T) or R(H) in FIG.", "OPH660.dat", "", "Internal field effect on vortex states in the layered organic superconductor lambda-(BETS)2Fe1-xGaxCl4 (x = 0.37)", "2017", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan", "Phys.Rev.B, 95(2017)165133", "S. Uji,T. Terashima,T. Konoike,T. Yamaguchi,S. Yasuzuka,A. Kobayashi,B. Zhou", "", "" ] }, { "id": "661", "line_start": 536, "line_end": 536, "sha256": "347ae4e33058d70cc040fb317b29971c9b90486a5bfaeaca4ede254c47cb9540", "values": [ "661", "JPS086014706", "4-Feb", "kappa-(BETS)2FeBr4", "", "BETS", "", "", "", "", "", "", "1.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "2.5", "OPH661", "", "", "", "", "Tn, Tc determined by specific heat C(H,T) measurements. metamagnetic transition at 2 T. Pauli limit = 2.9 T. H-direction is important (anisotropy)", "OPH661.dat", "", "Anisotropic Field Dependence of the Superconducting Transition in the Magnetic Molecular Superconductor kappa-(BETS)2FeBr4", "2017", "", "Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan", "J.Phys.Soc.Jpn, 86(2017)014706", "Shuhei Fukuoka,Satoshi Yamashita,Yasuhiro Nakazawa,Takashi Yamamoto,Hideki Fujiwara", "", "" ] }, { "id": "662", "line_start": 537, "line_end": 537, "sha256": "1dba554e3c033305095ab1b2d9b2d816672cdf8c3338bf35409890f6812fb154", "values": [ "662", "ACS1180368", "FeCl4", "kappa-(BETS)2FeCl4", "", "BETS", "11.693", "35.945", "8.4914", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "not SC down to 2 K. R(2K)/R(300K) = 2E-4. Space-G = Pnma. Dens = 2.497 g/cm3. For T=10K, a=11.483, b=35.720, c=8.383. Dens = 2.593 g/cm3", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "663", "line_start": 538, "line_end": 538, "sha256": "20ebf35e8a78dd00be296324668adc9fd7ac72a656502f4792c4c44451e8fb52", "values": [ "663", "ACS1180368", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "16.164", "18.538", "6.5928", "98.4", "96.67", "112.52", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OTMI663", "", "", "", "", "not SC down to 2 K. space-G = P1[-]. FIG shows P-dependence of MI transition. d=2.514 g/cm3. For 10K, a=15.890, b=18.378, c=6.531, alpha=98.61, beta=96.67, gamma= 112.05, d = 52.598 g/cm3", "OTMI663.dat", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "664", "line_start": 539, "line_end": 539, "sha256": "3fe36825811b1765d715cf60ecb81cc4f5547b332d50e58b0975415460f84f37", "values": [ "664", "ACS1180368", "(Fe,Ga)Cl4", "ramda-(BETS)2Fe0.48Ga0.52Cl4", "", "BETS", "", "", "", "", "", "", "4.6", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Ga-content by EPMA", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "665", "line_start": 540, "line_end": 540, "sha256": "fcae0d291cd5affa40b5068304b9498fe78f0d774c8ccd37fe6e6e7e94c73f50", "values": [ "665", "JPS086084704", "SbF6", "beta-(BDA-TTP)2SbF6", "", "BDA-TTP", "", "", "", "", "", "", "7.2", "", "", "", "", "", "", "", "", "", "12", "", "133", "", "", "", "", "", "", "", "", "OHC665", "OCOH665", "", "", "", "RRR(R300/R10) > 300. Inter layer distance = 17.6 A. Hc2 defined as R = 0.5Rn. cohere = 133 and 21 A for // and /n/ at 1.5 K. Aniso(Hc2) = 5.8 at 1.5 K. Inplane (ac-plane) anisotropy also measured.", "OHC665.dat", "OCOH665.dat", "Dimensional Crossover and Its Interplay with In-Plane Anisotropy of Upper Critical Field in beta-(BDA-TTP)2SbF6", "2017", "", "Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan", "J.Phys.Soc.Jpn, 86(2017)084704", "Syuma Yasuzuka,Hiroaki Koga,Yasuhisa Yamamura,Kazuya Saito,Shinya Uji,Taichi Terashima,Hiroki Akutsu,Jun-ichi Yamada", "", "" ] }, { "id": "666", "line_start": 541, "line_end": 541, "sha256": "77918e89cb1fca43549b6e0e4a574d528454df7a2f327717cd244bf0626c2c0c", "values": [ "666", "ACS1180368", "CoCl4", "kappa-(BETS)2CoCl4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Mettalic for T > 2K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CoCl4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "667", "line_start": 542, "line_end": 542, "sha256": "135ebe3d56d550ebfd5203214e0fa1ee7b699bf08f048eede1d394b55fbcf9c7", "values": [ "667", "ACS1180368", "MnCl4", "(BETS)2MnCl4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at about 40 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnCl4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "668", "line_start": 543, "line_end": 543, "sha256": "2dd2a56691a3b42a378b513b714213da5d4a5db2531679d251a62b672b126744", "values": [ "668", "ACS1180368", "MnBr4", "(BETS)2MnBr4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at about 70 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnBr4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "669", "line_start": 544, "line_end": 544, "sha256": "767e601e0755c77be2713881d94ceab3e545fbb5167f5d38a0814fa8bc237adb", "values": [ "669", "ACS1180368", "NiCl4", "(BETS)2NiCl4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at about 50 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)NiCl4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "670", "line_start": 545, "line_end": 545, "sha256": "5e97fe64a929dcac43d34c66bf147893d05d4a16d79d595d92acf0c292d4c75c", "values": [ "670", "ACS1180368", "CuCl4", "(BETS)2CuCl4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Metallic for T > 4 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuCl4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "671", "line_start": 546, "line_end": 546, "sha256": "eb0eb18b4d99e419a5f9d6afc20ad0ef6ce320a1c9a621e9efcf3ab55e6a1a38", "values": [ "671", "ACS1180368", "CuBr4", "(BETS)2CuBr4", "", "BETS", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "M-I transition at about 55 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuBr4, solvent=TCE.", "", "", "New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)", "1996", "", "Institute for Molecular Science, Okazaki 444, Japan", "J.Am.Chem.Soc., 118(1996)368", "Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux", "", "" ] }, { "id": "675", "line_start": 547, "line_end": 547, "sha256": "25bbe2f5cc2b5fc54715921d728e153a44ba44d0fc385d95974825a0c177bdd3", "values": [ "675", "PRB097024505", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "9.5", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OHC675", "", "", "", "", "three phases: I(H<0.6T, R//=0 and R/n=0), II(0.60), III(4T,H,Hc2, R//>0 and R/n>0)", "OHC675.dat", "", "Quantum vortex melting and phase diagram in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2", "2018", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan", "Phys.Rev.B, 97(2018)024505", "S. Uji,Y. Fujii,S. Sugiura,T. Terashima,T. Isono,J. Yamada", "", "" ] }, { "id": "676", "line_start": 548, "line_end": 548, "sha256": "3f15e23035a2f499a8b0974df2e342019a37af4c6e25803526512c800a13c9d6", "values": [ "676", "PRB097144505", "[(H3O)Ga(C2O4)3]:PhNO2", "beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2", "", "BEDT-TTF", "10.2782", "19.8733", "35.043", "", "93.423", "", "4.8", "", "", "0", "", "", "", "", "", "", "21", "", "", "", "", "", "", "", "", "", "", "OHC676", "", "", "", "", "Ph = C6H5. Hc2/n/ = 2.5 T. Hc2//=8.4*Hc2/n/. FFLO state sudied by measuring resistivity and torque. H = 15 T = 3.1Tc.", "OHC676.dat", "", "Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]C6H5NO2", "2018", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan", "Phys.Rev.B, 97(2018)144505", "S. Uji,Y. Iida,S. Sugiura,T. Isono,K. Sugii,N. Kikugawa,T. Terashima,S. Yasuzuka,H. Akutsu,Y. Nakazawa,D. Graf,P. Day", "", "" ] }, { "id": "677", "line_start": 549, "line_end": 549, "sha256": "e2ac2af81b5370c5dbc871561826fc23b7efd73db9959ace3103adcb153c2daf", "values": [ "677", "PRL116067003", "SF5CH2CF2SO3", "beta''-(BEDT-TTF)2SF5CH2CF2SO3", "", "BEDT-TTF", "", "", "", "", "", "", "5.2", "", "", "0", "", "", "", "", "", "", "14", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "From ref.16 in PRB097(2018)144505. Hc2/n/ = 1.3 T. Hc2//=11.5*Hc2/n/. H = 9.5 T = 1.9Tc.", "", "", "Microscopic Study of the Fulde-Ferrell-Larkin-Ovchinnikov State in an All-Organic Superconductor", "2016", "", "Department of Physics and Astronomy, UCLA, Los Angeles, California 90095, USA", "Phys.Rev.Lett., 116(2016)067003", "G. Koutroulakis,H. Kuhne,J.?A. Schlueter,J. Wosnitza,S.?E. Brown", "", "" ] }, { "id": "678", "line_start": 550, "line_end": 550, "sha256": "f80b240e06cbe97c3ca274668c0e90e449d91f05a8e8f40526b5ad2e0b9729d2", "values": [ "678", "PRB097224502", "EtMe3P", "EtMe3P[Pd(dmit)2]2", "", "[Pd(dmit)2", "", "", "", "", "", "", "4.36", "", "", "0", "", "", "", "", "", "", "", "2.7", "", "", "", "", "", "", "", "", "", "OHC678", "", "", "", "", "Et=C2H5, Me=CH3. Hc2(T) for H//plane. For H/n, (dHc2/dT) = (1/6)*2.7 (=value of dHc2/dT for H//plane). anisotropy factor m/m = 32. sample prepared by aerial oxidation method", "OHC678.dat", "", "Dimensionality of superconductivity in the layered organic material EtMe3P[Pd(dmit)2]2 under pressure", "2018", "", "Department of Applied Physics, Tokyo University of Science, Tokyo 125-8585, Japan", "Phys.Rev.B, 97(2018)224502", "R. Yamamoto,Y. Yanagita,T. Namaizawa,S. Komuro,T. Furukawa,T. Itou,R. Kato", "", "" ] }, { "id": "679", "line_start": 551, "line_end": 551, "sha256": "d598bb312033c438521fba1938a6e30f9947dca7e6e158b416f16e4a734ad7ed", "values": [ "679", "JPS085043705", "GaCl4", "ramda-(BETS)2GaCl4", "", "BETS", "", "", "", "", "", "", "4.8", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "4.3", "", "20.6", "", "", "", "", "", "", "", "", "gap 2d =4.30 kTc from SP. (dC/gamma*Tc) = 1.56. These data added to #652", "", "", "Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4", "2016", "", "Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan", "J.Phys.Soc.Jpn, 85(2016)043705", "Shusaku Imajo,Naoki Kanda,Satoshi Yamashita,Hiroki Akutsu,Yasuhiro Nakazawa,Hiroya Kumagai,Takuya Kobayashi,Atsushi Kawamoto", "", "" ] }, { "id": "680", "line_start": 552, "line_end": 552, "sha256": "d4ebb41c4d9b335dcfe443db7daae88f906fd7df4dfe14d6d8a002f5934530b7", "values": [ "680", "PRB098115111", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x: x=0.07", "", "TMTSF", "", "", "", "", "", "", "0.83", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)", "", "", "Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4", "2018", "", "Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria", "Phys.Rev.B, 98(2018)115111", "Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome", "", "" ] }, { "id": "681", "line_start": 553, "line_end": 553, "sha256": "67e6221b03c0e6bfd31b9d166450e80d084fc29d77a780b203a10d9ed4d710be", "values": [ "681", "PRB098115111", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x: x=0.06", "", "TMTSF", "", "", "", "", "", "", "0.77", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)", "", "", "Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4", "2018", "", "Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria", "Phys.Rev.B, 98(2018)115111", "Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome", "", "" ] }, { "id": "682", "line_start": 554, "line_end": 554, "sha256": "52f3898001a174c15e20ee126acb85e5d1f3270f2c453e595191a823194a7553", "values": [ "682", "PRB098115111", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x: x=0.1", "", "TMTSF", "", "", "", "", "", "", "0.39", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)", "", "", "Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4", "2018", "", "Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria", "Phys.Rev.B, 98(2018)115111", "Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome", "", "" ] }, { "id": "683", "line_start": 555, "line_end": 555, "sha256": "155bf7ce2c6115db6926c51884447e340e370063121b3a494a441b0d80630aab", "values": [ "683", "PRB098115111", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x: x = 0", "", "TMTSF", "", "", "", "", "", "", "1.58", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Kyoto-sample. Tc(zero) = 1.19 K", "", "", "Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4", "2018", "", "Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria", "Phys.Rev.B, 98(2018)115111", "Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome", "", "" ] }, { "id": "684", "line_start": 556, "line_end": 556, "sha256": "0a1eb21ab2d0f9f2dac070a32f343326a53936cfb63f864348d4c6b4314a7cba", "values": [ "684", "PRB098115111", "ClO4-ReO4", "(TMTSF)2(ClO4)1-x(ReO4)x: x = 0", "", "TMTSF", "", "", "", "", "", "", "1.35", "", "", "0", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Orsay-sample . Tc(zero) = 1.08 K. resistivity (along c* axis) larger than Kyoto-sample", "", "", "Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4", "2018", "", "Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria", "Phys.Rev.B, 98(2018)115111", "Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome", "", "" ] }, { "id": "685", "line_start": 557, "line_end": 557, "sha256": "eb862aa1ac0aa9999afdf9b98ea22c8c3aeba4c6f136494d1ac7be484ed72059", "values": [ "685", "PRB0610750", "Cu(NCS)2", "kappa-(BEDT-TTF)2Cu(NCS)2", "", "BEDT-TTF", "", "", "", "", "", "", "10.2", "", "", "0", "", "", "", "", "", "", "30", "3", "", "", "", "", "", "", "", "", "", "OHC685A", "OHC685B", "", "", "", "Hc2 defined as R = 1 Ohm(Hc2) and R-cross point (H*). Boss diffinitions give the same (dHc2/dT) value. Pauli limit discussed in details", "OHC685A.dat", "OHC685B.dat", "Paramagnetic limiting of the upper critical field of the layered organic superconductor kappa -(BEDT-TTF)2Cu(SCN)2", "2000", "", "Department of Physics, University of Miami, Coral Gables, Florida 33124", "Phys.Rev.B, 61(2000)750", "F. Zuo,J. S. Brooks,Ross H. McKenzie,J. A. Schlueter,Jack M. Williams", "", "" ] }, { "id": "686", "line_start": 558, "line_end": 558, "sha256": "9e041c4d679038326bcd8fdafcab9572420e13f98b0e52b4d7c6377eeb7ff955", "values": [ "686", "PRB085174530", "FeCl4", "ramda-(BETS)2FeCl4", "", "BETS", "", "", "", "", "", "", "2.1", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH686", "", "", "", "", "H-induced SC. Tc(in DB) shows tricritical point. FFLO state appears in SC region. Phase diagram shows for H//c.", "OPH686.dat", "", "Magnetic torque studies on FFLO phase in magnetic-field-induced organic superconductor lambda-(BETS)2FeCl4", "2012", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B, 85(2012)174530", "S. Uji,K. Kodama,K. Sugii,T. Terashima,Y. Takahide,N. Kurita,S. Tsuchiya,M. Kimata,A. Kobayashi,B. Zhou,H. Kobayashi", "", "" ] }, { "id": "687", "line_start": 559, "line_end": 559, "sha256": "aa8cf830eac8890ae7665013b38f8b02e55ed32ee91a5233cccbe9232e056581", "values": [ "687", "JPS087123704", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "", "BEDT-TTF", "", "", "", "", "", "", "12", "", "", "0", "", "", "", "", "", "", "7", "0.6", "70", "", "", "", "", "", "", "", "", "OHC687-1", "OHC687-2", "", "", "", "Hc2,dHc2/dT for H/n/plane. cohere//, cohere/n/ = 3 A. out-of-plane resistance (I//b-axis) measured. C/gamma*Tc = 3.3", "OHC687-1.dat", "OHC687-2.dat", "Superconducting Phase Diagram of the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br above 30T", "2018", "", "The Institute for Solid State Physics, the University of Tokyo, Kashiwa, Chiba 277-8581, Japan", "J.Phys.Soc.Jpn, 87(2018)123704", "Shusaku Imajo,Yasuhiro Nakazawa,Koichi Kindo", "", "" ] }, { "id": "700", "line_start": 560, "line_end": 560, "sha256": "be05fc9e8a259ea02e453ffaa7ed1a603898087bcbf37262ffd08e4239a05767", "values": [ "700", "PRB100014515", "SF5CH2CF2SO3", "(beta)''-(BEDT-TTF)2SF5CH2CF2SO3", "3", "BEDT-TTF", "", "", "", "", "", "", "5.2", "", "", "", "", "", "", "", "", "", "14", "", "", "", "", "", "", "", "", "", "", "OHC700", "", "", "", "", "Tc = 4.7 - 5.2 K. Hc2//ab = 14 T, Hc2/n/ab = 1.3 T. H = 9.5 - 10 T. T/Tc = 1.9 - 2.1 T/K.", "OHC700.dat", "", "Josephson vortex dynamics and Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta-(BEDT-TTF)2SF5CH2CF2SO3", "2019", "", "National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan", "Phys.Rev.B., 100(2019)014515", "Shiori Sugiura,Taichi Terashima,Shinya Uji,Syuma Yasuzuka,John A. Schlueter", "", "" ] }, { "id": "1001", "line_start": 561, "line_end": 561, "sha256": "6aa297969ce3715d4967d05f8b72ff4b7bc31aa9eeebbe837e7296a0965a41f3", "values": [ "1001", "PR05703623", "NH4Hg(SCN)4", "alpha-(BEDT-TTF)2NH4Hg(SCN)4", "3", "BEDT-TTF", "", "", "", "", "", "", "0.95", "", "", "", "", "", "", "", "", "", "", "0.08", "500", "0.7", "", "", "", "", "", "", "", "", "", "specific heat C/T vs T", "", "", "out-of-plane coherence = 1400 micron. Anysotropy factor=2000. Inter layer spacing=20 A.", "", "", "Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy", "1998", "", "Institute for Molecular Science, Myodaiji, Okazaki 444, Japan", "Phys.Rev.B,57(1998)3623", "H.Taniguchi,Hiromi Taniguchi,K.Kanoda,Kazushi Kanoda,Y.Nakazawa,Yasuhiro Nakazawa", "", "" ] }, { "id": "1002", "line_start": 562, "line_end": 562, "sha256": "10526c2cc27528c4d839c3a60a298318eaa6ac60b7bc7d6deac027d0f75a0f2a", "values": [ "1002", "JPS0652987", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "3", "BEDT-TTF", "", "", "", "", "", "", "12.6", "12.6", "", "0.019", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH1002", "", "phase diagram", "", "", "hydrogenated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=19 MPa. SC-1 to SC at P=30 MPa.", "OPH1002.dat", "", "Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure", "1996", "", "Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 65(1996)2987", "H.Ito,T.Ishiguro,M.Kubota,G.Saito", "", "" ] }, { "id": "1003", "line_start": 563, "line_end": 563, "sha256": "88a8983593ab49cae300ccb15025da626c8e58cf4e1e7ce2fab1933992d9e7be", "values": [ "1003", "JPS0652987", "Cu[N(CN)2]Cl", "kappa-(BEDT-TTF)2Cu[N(CN)2]Cl", "3", "BEDT-TTF", "", "", "", "", "", "", "13", "13", "", "0.034", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "OPH1003", "", "phase diagram", "", "", "deuterated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=34 MPa. SC-1 to SC at P=44 MPa.", "OPH1003.dat", "", "Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure", "1996", "", "Kyoto University, Kyoto,Japan", "J.Phys.Soc.Jpn, 65(1996)2987", "H.Ito,T.Ishiguro,M.Kubota,G.Saito", "", "" ] }, { "id": "1004", "line_start": 564, "line_end": 564, "sha256": "8e940d078b2eed3d9021e5ef3f40fb8e4591967fdb638c085da9f0219ea9b0f8", "values": [ "1004", "PR05705610", "Cu[N(CN)2]Br", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "BEDT-TTF", "", "", "", "", "", "", "11.5", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "isothermal magnetoresistance", "", "", "R has a peak at Hc(on). -dHc2/dT=0.7 T/K if the peak field is Hc2.", "", "", "Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br", "1998", "", "Department of Physics, University of Miami, Coral Gables, florida 33124", "Phys.Rev.B,57(1998)R5610-R5613", "F. Zuo,F.Zuo,J.A. Schlueter,J.A.Schlueter,J.M.Williams,Jack M. Williams,M.E. Kelly,M.E.Kelly,P. Zhang,P.Zhang,X. Su,X.Su", "", "" ] }, { "id": "1005", "line_start": 565, "line_end": 565, "sha256": "c1d0a8f0ab643c2a60ee7fd6fdbec26466fc12b9f7a8f2296a443c9c9dd85d82", "values": [ "1005", "ANC570146", "Cu-BHT", "[Cu3(C6S6)]n", "5", "monoclinic, C2", "15.016", "8.691", "3.489", "", "", "", "0.26", "3", "", "", "", "", "", "", "", "", "2500", "", "360", "", "", "", "", "15.1", "156.5", "", "", "001005fig1", "001005fig2", "", "", "", "The first observation of superconductivity in the coordination polymer. From the superconducting volume fraction of the bulk samples, mono- or few layers is suggested to show Tc of about 3K.", "001005fig1.csv", "001005fig2.csv", "Superconductivity in a Copper(II)-based coordination polymer with perfect Kagome structure", "2017", "coordination polymer, kagome lattice, quantum criticality, quantum spin liquid, superconductivity", "Beijing National Laboratory for Molecular Sciences, Key Laboratory of Organic Solids, Insitute of Chemistry, Chinese Academy of Science, Beijing 100190, China", "Angewandte Chemie, International Edition, 57(2018)146", "X. Huang,S. Zhang,L. Liu,L. Yu,G. Chen,W. Xu,D. Zhu", "", "" ] }, { "id": "1006", "line_start": 566, "line_end": 566, "sha256": "7e8cd74cc68ab55efda444d80935116d042d65de3e0930506e896ee7810c44c9", "values": [ "1006", "PRR01033184", "beta\"-[BEDT-TTF]", "beta\"-[BEDT-TTF]4[(H3O)M(C2O4)3]G", "1", "monoclinic, C2", "", "", "", "", "", "", "0", "7.2", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "001006fig1", "", "", "001006TBL1", "", "From the chemical substitution of guest organic to the beatha-type salts, Tc is influenced by the b-axis length, in which the charge disproportionation is caused by the stronger electron correlation.", "001006fig1.csv", "", "Effects of electron correlations and chemical pressures on superconductivity of beta\"-type organic compounds", "2019", "beta\"-type, organic superconductor, superconductivity, chemical pressure", "Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan", "Physical Review Research, 1(2019)033184", "S. Imajo,H. Akutsu,A. Akutsu-Sato,A. L. Morritt,L. Martin,Y. Nakazawa", "", "" ] }, { "id": "1007", "line_start": 567, "line_end": 567, "sha256": "090155298a6a54ad0accf373eaccf7e981d99b7bc7822d680e62fe765562f279", "values": [ "1007", "NAT4640076", "", "K2.9-picene", "", "picene", "8.707", "5.912", "12.97", "", "92.77", "", "7", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "K-doped picene. SC-volume fraction = 0.1 %. alkali-metal doping by annealing (440K, 9.0 days).", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "1008", "line_start": 568, "line_end": 568, "sha256": "6811f1d9ca49c1ccb992fdabe20326df49df571f377c0b992386f52a067db3be", "values": [ "1008", "NAT4640076", "", "K3.3-picene", "", "picene", "", "", "", "", "", "", "18", "", "", "", "", "", "", "", "", "38", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "K-doped picene. SC-volume fraction = 1.2 %. Hc1 at 5 K. alkali-metal doping by annealing (440K, 11 days).", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "1009", "line_start": 569, "line_end": 569, "sha256": "966ec2081af57dc4d271cb62254b4f7553b176f22d60049a78c4e923e1a082b4", "values": [ "1009", "NAT4640076", "", "Rb3.1-picene", "", "picene", "", "", "", "", "", "", "6.9", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "Rb-doped picene. SC-volume fraction = 10 %. alkali-metal doping by annealing (570K, 6.7 days).", "", "", "Superconductivity in alkali-metal-doped picene", "2010", "", "Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan", "Nature, 464(2010)76", "Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono", "", "" ] }, { "id": "1010", "line_start": 570, "line_end": 570, "sha256": "c04432d8a45149bc28744e6fccbc859e81c58aed10a7c54e49724c6360e60203", "values": [ "1010", "PRX010031028", "k-BEDT-TTF", "kappa-(BEDT-TTF)2Cu[N(CN)2]Br", "3", "", "", "", "", "", "", "", "12.5", "50", "", "", "3", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "", "001007fig1", "001007fig2", "", "", "", "Photot-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.", "", "", "Photomolecular high-temperature superconductivity", "2020", "k-(BEDT-TTF)2cu[N(CN)2]Br, light, photomolecular", "Max Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany", "Physical Review X10(2020)031028", "M. Buzzi,D. Nicoletti,M. Fechner,N. Tancogne-Dejean,M.A. Sentef,A. Georges,T. Biesner,E. Uykur,M. Dessel,A. Henderson,T. Siegrist,J.A. Schlawin,K. Miyagawa,K. Kanoda,M.-S. Nam,A. Ardavan,J. Coulthard,J. Tindall,F. Schlawin,A. Cavalleri", "k-(BEDT-TTF)2cu[N(CN)2]Br", "Photo-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K." ] } ] }