Organic source references

Explore reported properties, pressure context and source remarks from NIMS MDR SuperCon, version 240322.

Names, remarks or referenceSource structure labelHas source field

Search uses original source text. Rows remain separate references; catalogue sample associations are unestablished.

568 matching source rows · 561–568 shown

Only pcrit explicitly supplies GPa; the other numeric columns lack unit fields. Tc, maximum Tc and non-SC limits stay separate. A dash means no supplied value.

Organic source rows with separate transition and pressure columns; raw units are not inferred
Source material	Transition values (raw)	Pressure context	Reference / method
kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 1003 · BEDT-TTF	Tc 13 Maximum Tc 13	Critical pressure, pcrit 0.034 GPa	1996 · JPS0652987 Method —
Inspect row 1003: properties, remarks and source Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure J.Phys.Soc.Jpn, 65(1996)2987 Source remark: 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. Common name (raw) Cu[N(CN)2]Cl Sample form Single crystal bulk (code 3) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 563–563; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `88a8983593ab49cae300ccb15025da626c8e58cf4e1e7ce2fab1933992d9e7be` data number · `num` 1003 reference number · `refno` JPS0652987 common formula of materials · `name` Cu[N(CN)2]Cl full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Cl shape · `shape` 3 structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 13 maximum tc under pressure · `tcmax` 13 applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0.034 tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OPH1003 figure2 filename · `fig2` — figure description · `figname` phase diagram table file name · `tbl` — table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` OPH1003.dat f2 data file name · `f2_filename` — title · `title` Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure year · `year` 1996 keyword · `keyword` — institute · `institute` Kyoto University, Kyoto,Japan journal · `journal` J.Phys.Soc.Jpn, 65(1996)2987 author · `author` H.Ito,T.Ishiguro,M.Kubota,G.Saito sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 1004 · BEDT-TTF	Tc 11.5	—	1998 · PR05705610 Method —
Inspect row 1004: properties, remarks and source Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br Phys.Rev.B,57(1998)R5610-R5613 Source remark: R has a peak at Hc(on). -dHc2/dT=0.7 T/K if the peak field is Hc2. Common name (raw) Cu[N(CN)2]Br Sample form Single crystal bulk (code 3) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 564–564; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `8e940d078b2eed3d9021e5ef3f40fb8e4591967fdb638c085da9f0219ea9b0f8` data number · `num` 1004 reference number · `refno` PR05705610 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` 3 structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 11.5 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` isothermal magnetoresistance table file name · `tbl` — table description · `tblname` — comment · `commt` R has a peak at Hc(on). -dHc2/dT=0.7 T/K if the peak field is Hc2. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br year · `year` 1998 keyword · `keyword` — institute · `institute` Department of Physics, University of Miami, Coral Gables, florida 33124 journal · `journal` Phys.Rev.B,57(1998)R5610-R5613 author · `author` 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 sample · `sample` — comments · `comments` —
[Cu3(C6S6)]nRow 1005 · monoclinic, C2	Tc 0.26 Maximum Tc 3	—	2017 · ANC570146 Method —
Inspect row 1005: properties, remarks and source Superconductivity in a Copper(II)-based coordination polymer with perfect Kagome structure Angewandte Chemie, International Edition, 57(2018)146 Source remark: 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. Common name (raw) Cu-BHT Sample form Film (single) (code 5) Lattice a (raw) 15.016 Lattice b (raw) 8.691 Lattice c (raw) 3.489 Hc2 at 0 K (raw) 2500 Coherence length at 0 K (raw) 360 Electronic specific heat coefficient (raw) 15.1 Debye temperature (raw) 156.5 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 565–565; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `c1d0a8f0ab643c2a60ee7fd6fdbec26466fc12b9f7a8f2296a443c9c9dd85d82` data number · `num` 1005 reference number · `refno` ANC570146 common formula of materials · `name` Cu-BHT full material name · `fullname` [Cu3(C6S6)]n shape · `shape` 5 structure · `str` monoclinic, C2 lattice constant a · `lata` 15.016 lattice constant b · `latb` 8.691 lattice constant c · `latc` 3.489 lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0.26 maximum tc under pressure · `tcmax` 3 applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` 2500 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 360 penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` 15.1 Debye temperature · `debyet` 156.5 Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` 001005fig1 figure2 filename · `fig2` 001005fig2 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` 001005fig1.csv f2 data file name · `f2_filename` 001005fig2.csv title · `title` Superconductivity in a Copper(II)-based coordination polymer with perfect Kagome structure year · `year` 2017 keyword · `keyword` coordination polymer, kagome lattice, quantum criticality, quantum spin liquid, superconductivity institute · `institute` Beijing National Laboratory for Molecular Sciences, Key Laboratory of Organic Solids, Insitute of Chemistry, Chinese Academy of Science, Beijing 100190, China journal · `journal` Angewandte Chemie, International Edition, 57(2018)146 author · `author` X. Huang,S. Zhang,L. Liu,L. Yu,G. Chen,W. Xu,D. Zhu sample · `sample` — comments · `comments` —
beta"-[BEDT-TTF]4[(H3O)M(C2O4)3]GRow 1006 · monoclinic, C2	Tc 0 Maximum Tc 7.2	—	2019 · PRR01033184 Method —
Inspect row 1006: properties, remarks and source Effects of electron correlations and chemical pressures on superconductivity of beta"-type organic compounds Physical Review Research, 1(2019)033184 Source remark: 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. Common name (raw) beta"-[BEDT-TTF] Sample form Single phase bulk (code 1) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 566–566; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `7e8cd74cc68ab55efda444d80935116d042d65de3e0930506e896ee7810c44c9` data number · `num` 1006 reference number · `refno` PRR01033184 common formula of materials · `name` beta"-[BEDT-TTF] full material name · `fullname` beta"-[BEDT-TTF]4[(H3O)M(C2O4)3]G shape · `shape` 1 structure · `str` monoclinic, C2 lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0 maximum tc under pressure · `tcmax` 7.2 applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` 001006fig1 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` 001006TBL1 table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` 001006fig1.csv f2 data file name · `f2_filename` — title · `title` Effects of electron correlations and chemical pressures on superconductivity of beta"-type organic compounds year · `year` 2019 keyword · `keyword` beta"-type, organic superconductor, superconductivity, chemical pressure institute · `institute` Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan journal · `journal` Physical Review Research, 1(2019)033184 author · `author` S. Imajo,H. Akutsu,A. Akutsu-Sato,A. L. Morritt,L. Martin,Y. Nakazawa sample · `sample` — comments · `comments` —
K2.9-piceneRow 1007 · picene	Tc 7	—	2010 · NAT4640076 Method —
Inspect row 1007: properties, remarks and source Superconductivity in alkali-metal-doped picene Nature, 464(2010)76 Source remark: K-doped picene. SC-volume fraction = 0.1 %. alkali-metal doping by annealing (440K, 9.0 days). Common name (raw) Not supplied Sample form Not supplied Lattice a (raw) 8.707 Lattice b (raw) 5.912 Lattice c (raw) 12.97 Lattice β (raw) 92.77 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 567–567; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `090155298a6a54ad0accf373eaccf7e981d99b7bc7822d680e62fe765562f279` data number · `num` 1007 reference number · `refno` NAT4640076 common formula of materials · `name` — full material name · `fullname` K2.9-picene shape · `shape` — structure · `str` picene lattice constant a · `lata` 8.707 lattice constant b · `latb` 5.912 lattice constant c · `latc` 12.97 lattice alpha · `alpha` — lattice beta · `beta` 92.77 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 7 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` K-doped picene. SC-volume fraction = 0.1 %. alkali-metal doping by annealing (440K, 9.0 days). figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in alkali-metal-doped picene year · `year` 2010 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Nature, 464(2010)76 author · `author` Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono sample · `sample` — comments · `comments` —
K3.3-piceneRow 1008 · picene	Tc 18	—	2010 · NAT4640076 Method —
Inspect row 1008: properties, remarks and source Superconductivity in alkali-metal-doped picene Nature, 464(2010)76 Source remark: K-doped picene. SC-volume fraction = 1.2 %. Hc1 at 5 K. alkali-metal doping by annealing (440K, 11 days). Common name (raw) Not supplied Sample form Not supplied Hc1 at 0 K (raw) 38 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 568–568; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6811f1d9ca49c1ccb992fdabe20326df49df571f377c0b992386f52a067db3be` data number · `num` 1008 reference number · `refno` NAT4640076 common formula of materials · `name` — full material name · `fullname` K3.3-picene shape · `shape` — structure · `str` picene lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 18 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` 38 Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` K-doped picene. SC-volume fraction = 1.2 %. Hc1 at 5 K. alkali-metal doping by annealing (440K, 11 days). figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in alkali-metal-doped picene year · `year` 2010 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Nature, 464(2010)76 author · `author` Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono sample · `sample` — comments · `comments` —
Rb3.1-piceneRow 1009 · picene	Tc 6.9	—	2010 · NAT4640076 Method —
Inspect row 1009: properties, remarks and source Superconductivity in alkali-metal-doped picene Nature, 464(2010)76 Source remark: Rb-doped picene. SC-volume fraction = 10 %. alkali-metal doping by annealing (570K, 6.7 days). Common name (raw) Not supplied Sample form Not supplied Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 569–569; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `966ec2081af57dc4d271cb62254b4f7553b176f22d60049a78c4e923e1a082b4` data number · `num` 1009 reference number · `refno` NAT4640076 common formula of materials · `name` — full material name · `fullname` Rb3.1-picene shape · `shape` — structure · `str` picene lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 6.9 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Rb-doped picene. SC-volume fraction = 10 %. alkali-metal doping by annealing (570K, 6.7 days). figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in alkali-metal-doped picene year · `year` 2010 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Nature, 464(2010)76 author · `author` Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 1010 · Structure label not suppliedSample label: k-(BEDT-TTF)2cu[N(CN)2]Br	Tc 12.5 Maximum Tc 50	—	2020 · PRX010031028 Resistivity (code 3)
Inspect row 1010: properties, remarks and source Photomolecular high-temperature superconductivity Physical Review X10(2020)031028 Source remark: Photot-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K. Additional comment: Photo-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K. Common name (raw) k-BEDT-TTF Sample form Single crystal bulk (code 3) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 570–570; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `c04432d8a45149bc28744e6fccbc859e81c58aed10a7c54e49724c6360e60203` data number · `num` 1010 reference number · `refno` PRX010031028 common formula of materials · `name` k-BEDT-TTF full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` 3 structure · `str` — lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 12.5 maximum tc under pressure · `tcmax` 50 applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` 3 alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` 001007fig1 figure2 filename · `fig2` 001007fig2 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Photot-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Photomolecular high-temperature superconductivity year · `year` 2020 keyword · `keyword` k-(BEDT-TTF)2cu[N(CN)2]Br, light, photomolecular institute · `institute` Max Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany journal · `journal` Physical Review X10(2020)031028 author · `author` 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 sample · `sample` k-(BEDT-TTF)2cu[N(CN)2]Br comments · `comments` Photo-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.

Dataset coverage, units and downloads

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. Dataset version · CC BY 4.0.

568 nonempty source rows, 49 original columns. One all-empty trailing row is excluded and recorded in the manifest. Source row counts are not material or independent-experiment counts. Publication status and catalogue sample/phase associations have not been checked.

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. Maximum Tc under pressure; pmax is its associated applied pressure, unlike the oxide/metallic table pmax definition. Lowest measurement temperature for a non-superconducting report, not a Tc value.

Numeric cells are not converted or assigned absent units. Comments can contain additional conditions or units and remain source text. Guide code labels are provided for sample form and measurement methods; raw codes remain available.

Full reference JSON JSON SHA-256 Original table bytes

Source file SHA-256: d116848a90d01e48356ed6cf0bb69035fa863a3a559deac1ef188025bdb3b423

Tc (critical / atmospheric pressure): 517 nonempty rows
Maximum Tc under pressure: 83 nonempty rows
Critical pressure (GPa): 484 nonempty rows
Pressure at maximum Tc (raw): 74 nonempty rows
Non-SC test temperature limit: 23 nonempty rows
Tc method: 39 nonempty rows
Lattice a: 109 nonempty rows
Lattice b: 107 nonempty rows
Lattice c: 109 nonempty rows
Lattice α: 42 nonempty rows
Lattice β: 84 nonempty rows
Lattice γ: 42 nonempty rows
Isotope exponent: 28 nonempty rows
Isotope element: 52 nonempty rows
dTc/dP at P = 0: 53 nonempty rows
Hc1 at 0 K: 21 nonempty rows
Hc2 at 0 K: 70 nonempty rows
−dHc2/dT at Tc: 37 nonempty rows
Coherence length at 0 K: 73 nonempty rows
Penetration depth at 0 K: 41 nonempty rows
GL parameter (source glpar): 10 nonempty rows
Energy gap at 0 K: 15 nonempty rows
Gap method: 9 nonempty rows
Electronic specific heat coefficient: 31 nonempty rows
Debye temperature: 24 nonempty rows
Curie temperature: 10 nonempty rows
Néel temperature: 20 nonempty rows

Source material

Transition values (raw)

Pressure context

Reference / method

kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 1003 · BEDT-TTF

Tc: 13
Maximum Tc: 13

Critical pressure, pcrit: 0.034 GPa

1996 · JPS0652987

Method —

Inspect row 1003: properties, remarks and source

Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure

J.Phys.Soc.Jpn, 65(1996)2987

Source remark: 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.

Common name (raw): Cu[N(CN)2]Cl
Sample form: Single crystal bulk (code 3)

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 563–563; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 88a8983593ab49cae300ccb15025da626c8e58cf4e1e7ce2fab1933992d9e7be

data number · num: 1003
reference number · refno: JPS0652987
common formula of materials · name: Cu[N(CN)2]Cl
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Cl
shape · shape: 3
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 13
maximum tc under pressure · tcmax: 13
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0.034
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OPH1003
figure2 filename · fig2: —
figure description · figname: phase diagram
table file name · tbl: —
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: OPH1003.dat
f2 data file name · f2_filename: —
title · title: Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure
year · year: 1996
keyword · keyword: —
institute · institute: Kyoto University, Kyoto,Japan
journal · journal: J.Phys.Soc.Jpn, 65(1996)2987
author · author: H.Ito,T.Ishiguro,M.Kubota,G.Saito
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 1004 · BEDT-TTF

Tc: 11.5

—

1998 · PR05705610

Method —

Inspect row 1004: properties, remarks and source

Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br

Phys.Rev.B,57(1998)R5610-R5613

Source remark: R has a peak at Hc(on). -dHc2/dT=0.7 T/K if the peak field is Hc2.

Common name (raw): Cu[N(CN)2]Br
Sample form: Single crystal bulk (code 3)

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 564–564; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 8e940d078b2eed3d9021e5ef3f40fb8e4591967fdb638c085da9f0219ea9b0f8

data number · num: 1004
reference number · refno: PR05705610
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: 3
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 11.5
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: isothermal magnetoresistance
table file name · tbl: —
table description · tblname: —
comment · commt: R has a peak at Hc(on). -dHc2/dT=0.7 T/K if the peak field is Hc2.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Effects of inhomogeneity on the interlayer magnetresistance in the organic superconductor k-(BEDT-TTF)2Cu[N(CN)2]Br
year · year: 1998
keyword · keyword: —
institute · institute: Department of Physics, University of Miami, Coral Gables, florida 33124
journal · journal: Phys.Rev.B,57(1998)R5610-R5613
author · author: 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
sample · sample: —
comments · comments: —

[Cu3(C6S6)]nRow 1005 · monoclinic, C2

Tc: 0.26
Maximum Tc: 3

—

2017 · ANC570146

Method —

Inspect row 1005: properties, remarks and source

Superconductivity in a Copper(II)-based coordination polymer with perfect Kagome structure

Angewandte Chemie, International Edition, 57(2018)146

Source remark: 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.

Common name (raw): Cu-BHT
Sample form: Film (single) (code 5)
Lattice a (raw): 15.016
Lattice b (raw): 8.691
Lattice c (raw): 3.489
Hc2 at 0 K (raw): 2500
Coherence length at 0 K (raw): 360
Electronic specific heat coefficient (raw): 15.1
Debye temperature (raw): 156.5

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All 49 original cells and provenance

Original physical lines 565–565; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: c1d0a8f0ab643c2a60ee7fd6fdbec26466fc12b9f7a8f2296a443c9c9dd85d82

data number · num: 1005
reference number · refno: ANC570146
common formula of materials · name: Cu-BHT
full material name · fullname: [Cu3(C6S6)]n
shape · shape: 5
structure · str: monoclinic, C2
lattice constant a · lata: 15.016
lattice constant b · latb: 8.691
lattice constant c · latc: 3.489
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0.26
maximum tc under pressure · tcmax: 3
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: 2500
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 360
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: 15.1
Debye temperature · debyet: 156.5
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: 001005fig1
figure2 filename · fig2: 001005fig2
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: 001005fig1.csv
f2 data file name · f2_filename: 001005fig2.csv
title · title: Superconductivity in a Copper(II)-based coordination polymer with perfect Kagome structure
year · year: 2017
keyword · keyword: coordination polymer, kagome lattice, quantum criticality, quantum spin liquid, superconductivity
institute · institute: Beijing National Laboratory for Molecular Sciences, Key Laboratory of Organic Solids, Insitute of Chemistry, Chinese Academy of Science, Beijing 100190, China
journal · journal: Angewandte Chemie, International Edition, 57(2018)146
author · author: X. Huang,S. Zhang,L. Liu,L. Yu,G. Chen,W. Xu,D. Zhu
sample · sample: —
comments · comments: —

beta"-[BEDT-TTF]4[(H3O)M(C2O4)3]GRow 1006 · monoclinic, C2

Tc: 0
Maximum Tc: 7.2

—

2019 · PRR01033184

Method —

Inspect row 1006: properties, remarks and source

Effects of electron correlations and chemical pressures on superconductivity of beta"-type organic compounds

Physical Review Research, 1(2019)033184

Source remark: 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.

Common name (raw): beta"-[BEDT-TTF]
Sample form: Single phase bulk (code 1)

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 566–566; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 7e8cd74cc68ab55efda444d80935116d042d65de3e0930506e896ee7810c44c9

data number · num: 1006
reference number · refno: PRR01033184
common formula of materials · name: beta"-[BEDT-TTF]
full material name · fullname: beta"-[BEDT-TTF]4[(H3O)M(C2O4)3]G
shape · shape: 1
structure · str: monoclinic, C2
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0
maximum tc under pressure · tcmax: 7.2
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: 001006fig1
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: 001006TBL1
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: 001006fig1.csv
f2 data file name · f2_filename: —
title · title: Effects of electron correlations and chemical pressures on superconductivity of beta"-type organic compounds
year · year: 2019
keyword · keyword: beta"-type, organic superconductor, superconductivity, chemical pressure
institute · institute: Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan
journal · journal: Physical Review Research, 1(2019)033184
author · author: S. Imajo,H. Akutsu,A. Akutsu-Sato,A. L. Morritt,L. Martin,Y. Nakazawa
sample · sample: —
comments · comments: —

K2.9-piceneRow 1007 · picene

Tc: 7

—

2010 · NAT4640076

Method —

Inspect row 1007: properties, remarks and source

Superconductivity in alkali-metal-doped picene

Nature, 464(2010)76

Source remark: K-doped picene. SC-volume fraction = 0.1 %. alkali-metal doping by annealing (440K, 9.0 days).

Common name (raw): Not supplied
Sample form: Not supplied
Lattice a (raw): 8.707
Lattice b (raw): 5.912
Lattice c (raw): 12.97
Lattice β (raw): 92.77

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 567–567; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 090155298a6a54ad0accf373eaccf7e981d99b7bc7822d680e62fe765562f279

data number · num: 1007
reference number · refno: NAT4640076
common formula of materials · name: —
full material name · fullname: K2.9-picene
shape · shape: —
structure · str: picene
lattice constant a · lata: 8.707
lattice constant b · latb: 5.912
lattice constant c · latc: 12.97
lattice alpha · alpha: —
lattice beta · beta: 92.77
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 7
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: K-doped picene. SC-volume fraction = 0.1 %. alkali-metal doping by annealing (440K, 9.0 days).
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in alkali-metal-doped picene
year · year: 2010
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Nature, 464(2010)76
author · author: Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono
sample · sample: —
comments · comments: —

K3.3-piceneRow 1008 · picene

Tc: 18

—

2010 · NAT4640076

Method —

Inspect row 1008: properties, remarks and source

Superconductivity in alkali-metal-doped picene

Nature, 464(2010)76

Source remark: K-doped picene. SC-volume fraction = 1.2 %. Hc1 at 5 K. alkali-metal doping by annealing (440K, 11 days).

Common name (raw): Not supplied
Sample form: Not supplied
Hc1 at 0 K (raw): 38

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All 49 original cells and provenance

Original physical lines 568–568; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6811f1d9ca49c1ccb992fdabe20326df49df571f377c0b992386f52a067db3be

data number · num: 1008
reference number · refno: NAT4640076
common formula of materials · name: —
full material name · fullname: K3.3-picene
shape · shape: —
structure · str: picene
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 18
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: 38
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: K-doped picene. SC-volume fraction = 1.2 %. Hc1 at 5 K. alkali-metal doping by annealing (440K, 11 days).
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in alkali-metal-doped picene
year · year: 2010
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Nature, 464(2010)76
author · author: Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono
sample · sample: —
comments · comments: —

Rb3.1-piceneRow 1009 · picene

Tc: 6.9

—

2010 · NAT4640076

Method —

Inspect row 1009: properties, remarks and source

Superconductivity in alkali-metal-doped picene

Nature, 464(2010)76

Source remark: Rb-doped picene. SC-volume fraction = 10 %. alkali-metal doping by annealing (570K, 6.7 days).

Common name (raw): Not supplied
Sample form: Not supplied

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 569–569; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 966ec2081af57dc4d271cb62254b4f7553b176f22d60049a78c4e923e1a082b4

data number · num: 1009
reference number · refno: NAT4640076
common formula of materials · name: —
full material name · fullname: Rb3.1-picene
shape · shape: —
structure · str: picene
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 6.9
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Rb-doped picene. SC-volume fraction = 10 %. alkali-metal doping by annealing (570K, 6.7 days).
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in alkali-metal-doped picene
year · year: 2010
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Nature, 464(2010)76
author · author: Ryoji Mitsuhashi,Yuta Suzuki,Yusuke Yamanari,Hiroki Mitamura,Takashi Kambe,Naoshi Ikeda,Hideki Okamoto,Akihiko Fujiwara,Minoru Yamaji,Naoko Kawasaki,Yutaka Maniwa,Yoshihiro Kubozono
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 1010 · Structure label not suppliedSample label: k-(BEDT-TTF)2cu[N(CN)2]Br

Tc: 12.5
Maximum Tc: 50

—

2020 · PRX010031028

Resistivity (code 3)

Inspect row 1010: properties, remarks and source

Photomolecular high-temperature superconductivity

Physical Review X10(2020)031028

Source remark: Photot-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.

Additional comment: Photo-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.

Common name (raw): k-BEDT-TTF
Sample form: Single crystal bulk (code 3)

Link to this source row Original NIMS table Field guide, page 9

All 49 original cells and provenance

Original physical lines 570–570; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: c04432d8a45149bc28744e6fccbc859e81c58aed10a7c54e49724c6360e60203

data number · num: 1010
reference number · refno: PRX010031028
common formula of materials · name: k-BEDT-TTF
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: 3
structure · str: —
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 12.5
maximum tc under pressure · tcmax: 50
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: 3
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: 001007fig1
figure2 filename · fig2: 001007fig2
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Photot-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Photomolecular high-temperature superconductivity
year · year: 2020
keyword · keyword: k-(BEDT-TTF)2cu[N(CN)2]Br, light, photomolecular
institute · institute: Max Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany
journal · journal: Physical Review X10(2020)031028
author · author: 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
sample · sample: k-(BEDT-TTF)2cu[N(CN)2]Br
comments · comments: Photo-induced state in the density of quasiparticles of the equillibrium metal is achieved to be a characteristic coherence temperature about 50K.