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 · 401–420 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-((ET)0.95(MT)0.05)2Cu(NCS)2Row 419 · BEDT-TTF	Tc 7.9	Critical pressure, pcrit 0 GPa	2007 · J076123705 Method —
Inspect row 419: properties, remarks and source Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2 J.Phys.Soc.Jpn, 76(2007)123705 Source remark: impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence. Common name (raw) Cu(NCS)2 Sample form Not supplied Coherence length at 0 K (raw) 66 Penetration depth at 0 K (raw) 0.465 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 403–403; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6c347bcb83ca47678756778c1ed3fc38a4a47ca8a67f38fcc73ee9e3abe26d85` data number · `num` 419 reference number · `refno` J076123705 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-((ET)0.95(MT)0.05)2Cu(NCS)2 shape · `shape` — 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` 7.9 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 66 penetration depth at 0 K for poly crystal · `penet` 0.465 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` OHC418 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence. figure1 data file name · `f1_filename` OHC418.dat f2 data file name · `f2_filename` — title · `title` Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2 year · `year` 2007 keyword · `keyword` — institute · `institute` Institute for Materials Research, Tohoku University, Sendai 980-8577 journal · `journal` J.Phys.Soc.Jpn, 76(2007)123705 author · `author` Naoki YONEYAMA,Takahiko SASAKI,Hajime OIZUMI,Norio KOBAYASHI sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 420 · BEDT-TTF	Tc 9.2	Critical pressure, pcrit 0 GPa	2004 · JPS0731290 Method —
Inspect row 420: properties, remarks and source 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) J.Phys.Soc.Jpn, 73(2004)1290 Source remark: Tc not depends on cooling rate. [penet] by magnetization. Common name (raw) Cu(NCS)2 Sample form Not supplied Penetration depth at 0 K (raw) 0.43 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 404–404; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `86f761985e986b2b5f6908abddba779139d7325d32ef57348e06ace60c79fbfa` data number · `num` 420 reference number · `refno` JPS0731290 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 shape · `shape` — 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` 9.2 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 0.43 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` OTC421 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Tc not depends on cooling rate. [penet] by magnetization. figure1 data file name · `f1_filename` OTC421.dat f2 data file name · `f2_filename` — title · `title` 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) year · `year` 2004 keyword · `keyword` — institute · `institute` Institute for Materials Research, Tohoku University, Sendai 980-8577 journal · `journal` J.Phys.Soc.Jpn, 73(2004)1290 author · `author` Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 421 · BEDT-TTF	Tc 11.7	Critical pressure, pcrit 0 GPa	2004 · JPS0731290 Method —
Inspect row 421: properties, remarks and source 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) J.Phys.Soc.Jpn, 73(2004)1290 Source remark: 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). Common name (raw) Cu[N(CN)2]Br Sample form Not supplied Penetration depth at 0 K (raw) 0.57 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 405–405; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `916e13e1b22990b5362cf327f3f27060b20f44adda0e65ef49344313552e8cec` data number · `num` 421 reference number · `refno` JPS0731290 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` — 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` 11.7 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 0.57 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` 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). figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` 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) year · `year` 2004 keyword · `keyword` — institute · `institute` Institute for Materials Research, Tohoku University, Sendai 980-8577 journal · `journal` J.Phys.Soc.Jpn, 73(2004)1290 author · `author` Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI sample · `sample` — comments · `comments` —
(MDT-TS)(AuI2)0.441Row 422 · MDT-TS	Tc 4.9 Maximum Tc 4.9	Critical pressure, pcrit 1.05 GPa At maximum Tc, pmax (raw) 1.27	2008 · P077224506 Method —
Inspect row 422: properties, remarks and source Antiferromagnetic ordering of the incommensurate organic superconductor (MDT-TS)(AuI2)0.441 with a high spin-flop field Phys.Rev.B, 77(2008)224506 Source remark: 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. Common name (raw) AuI2 Sample form Not supplied Néel temperature (raw) 50 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 406–406; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `edecd9350428d9fa017838b44b6e4426a831c69298b8899c1caecf931eb587ae` data number · `num` 422 reference number · `refno` P077224506 common formula of materials · `name` AuI2 full material name · `fullname` (MDT-TS)(AuI2)0.441 shape · `shape` — structure · `str` MDT-TS 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` 4.9 maximum tc under pressure · `tcmax` 4.9 applied pressure for tcmax · `pmax` 1.27 Critical pressure/GPa at which Tc can be observed · `pcrit` 1.05 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` 50 figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Antiferromagnetic ordering of the incommensurate organic superconductor (MDT-TS)(AuI2)0.441 with a high spin-flop field year · `year` 2008 keyword · `keyword` — institute · `institute` Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan journal · `journal` Phys.Rev.B, 77(2008)224506 author · `author` Tadashi Kawamoto,Yoshimasa Bando,Takehiko Mori,Takako Konoike,Yamaguchi Takahide,Taichi Terashima,Shinya Uji,Kazuo Takimiya,Tetsuo Otsubo sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 423 · BEDT-TTFSample label: organic	Tc 10.5	Critical pressure, pcrit 0 GPa	1994 · PR04912990 Method —
Inspect row 423: properties, remarks and source Magnetic penetration depth and fluxon-line dynamics in the organic superconductor k-[BEDT-TTF]2Cu[NCS]2 Phys.Rev.B, 49(1994)12990 Source remark: [penet] shows London [penet] calculated from muon-SR result (0.877 micron-m). Common name (raw) Cu(NCS)2 Sample form Single crystal bulk (code 3) Lattice a (raw) 16.248 Lattice b (raw) 8.44 Lattice c (raw) 13.124 Lattice β (raw) 110.3 Hc2 at 0 K (raw) 7 Coherence length at 0 K (raw) 70 Penetration depth at 0 K (raw) 0.768 GL parameter (source glpar) (raw) 125 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 407–407; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `7cabdbde396ea587ccc203e26dc9ea06e1570e16468010685abd9838277d4cff` data number · `num` 423 reference number · `refno` PR04912990 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 shape · `shape` 3 structure · `str` BEDT-TTF lattice constant a · `lata` 16.248 lattice constant b · `latb` 8.44 lattice constant c · `latc` 13.124 lattice alpha · `alpha` — lattice beta · `beta` 110.3 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 10.5 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 7 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 70 penetration depth at 0 K for poly crystal · `penet` 0.768 Ginzburg-Landau order parameter · `glpar` 125 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` [penet] shows London [penet] calculated from muon-SR result (0.877 micron-m). figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Magnetic penetration depth and fluxon-line dynamics in the organic superconductor k-[BEDT-TTF]2Cu[NCS]2 year · `year` 1994 keyword · `keyword` — institute · `institute` — journal · `journal` Phys.Rev.B, 49(1994)12990 author · `author` A.T.Fiory,D.Li.Williams,D.R.Harshman,E.Koster,I.Shinkoda,M.L.Kaplan,R.C.Haddon,T.Pfiz sample · `sample` organic comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 424 · BEDT-TTFSample label: ORGANIC	Tc 8.3	Critical pressure, pcrit 0 GPa	1994 · PR05013603 Method —
Inspect row 424: properties, remarks and source Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br Phys.Rev.B.,50(1994) 13603 Source remark: surface impedance. For out-of-plane, [penet] = 40 um and [cohere] = 5 A. Common name (raw) Cu(NCS)2 Sample form Single crystal bulk (code 3) Coherence length at 0 K (raw) 70 Penetration depth at 0 K (raw) 1.4 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 408–408; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `5a5901c7673091cb90ec32d19b815c71a4368d9ebbfe44b3759cc5ceb2e8beb9` data number · `num` 424 reference number · `refno` PR05013603 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 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` 8.3 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 70 penetration depth at 0 K for poly crystal · `penet` 1.4 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` surface impedance. For out-of-plane, [penet] = 40 um and [cohere] = 5 A. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br year · `year` 1994 keyword · `keyword` — institute · `institute` — journal · `journal` Phys.Rev.B.,50(1994) 13603 author · `author` G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein sample · `sample` ORGANIC comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 425 · BEDT-TTFSample label: ORGANIC	Tc 11.3	Critical pressure, pcrit 0 GPa	1994 · PR05013603 Method —
Inspect row 425: properties, remarks and source Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br Phys.Rev.B.,50(1994) 13603 Source remark: surface impedance. For out-of-plane, [penet] = 38 um and [cohere] = 6 A. Common name (raw) Cu[N(CN)2]Br Sample form Not supplied Coherence length at 0 K (raw) 37 Penetration depth at 0 K (raw) 1.5 Energy gap at 0 K (raw) 5 Gap method Surface impedance (code 7) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 409–409; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `293c7b9fb4209f15233db5e127f74ca4fb8729d683e730965456d10b50deefd4` data number · `num` 425 reference number · `refno` PR05013603 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` — 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` 11.3 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 37 penetration depth at 0 K for poly crystal · `penet` 1.5 Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` 5 method of measuring energy gap · `gapmeth` 7 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` surface impedance. For out-of-plane, [penet] = 38 um and [cohere] = 6 A. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br year · `year` 1994 keyword · `keyword` — institute · `institute` — journal · `journal` Phys.Rev.B.,50(1994) 13603 author · `author` G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein sample · `sample` ORGANIC comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 426 · BEDT-TTF	Tc 8.3	Critical pressure, pcrit 0 GPa	1993 · PR04711595 Method —
Inspect row 426: properties, remarks and source Microwave surface impedance of kappa-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene: Evidence for unconventional superconductivity Phys.Rev.B, 47(1993)11595 Source remark: surface impedance. Common name (raw) Cu(NCS)2 Sample form Single crystal bulk (code 3) Penetration depth at 0 K (raw) 2 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 410–410; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `9955797391059a044ead1848091972e69953e924d7c0e84bf9914627e0b4a0de` data number · `num` 426 reference number · `refno` PR04711595 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 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` 8.3 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 2 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` surface impedance. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Microwave surface impedance of kappa-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene: Evidence for unconventional superconductivity year · `year` 1993 keyword · `keyword` — institute · `institute` — journal · `journal` Phys.Rev.B, 47(1993)11595 author · `author` D.Achkir,M.Poirier,C.Bourbonnais,G.Quirion,C.Lenoir,D.Jerome sample · `sample` — comments · `comments` —
beta-(BDA-TTP)2SbF6Row 427 · BDA-TTP	Tc 7.32	Critical pressure, pcrit 0 GPa	2008 · PRB078172506 Method —
Inspect row 427: properties, remarks and source Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression Phys.Rev.B, 78(2008)172506 Source remark: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method. Common name (raw) SbF6 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 411–411; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `198249640426be9921506a85a0a618f169fc42675ff38678bb74a1427a6f2511` data number · `num` 427 reference number · `refno` PRB078172506 common formula of materials · `name` SbF6 full material name · `fullname` beta-(BDA-TTP)2SbF6 shape · `shape` 3 structure · `str` BDA-TTP 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` 7.32 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` OTC427 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method. figure1 data file name · `f1_filename` OTC427.dat f2 data file name · `f2_filename` — title · `title` Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression year · `year` 2008 keyword · `keyword` — institute · `institute` Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan journal · `journal` Phys.Rev.B, 78(2008)172506 author · `author` Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi sample · `sample` — comments · `comments` —
beta-(BDA-TTP)2AsF6Row 428 · BDA-TTP	Tc 6.92	Critical pressure, pcrit 0 GPa	2008 · PRB078172506 Method —
Inspect row 428: properties, remarks and source Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression Phys.Rev.B, 78(2008)172506 Source remark: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method. Common name (raw) AsF6 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 412–412; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `be4373483b740c351f7921e4d6f1676d0e970940b5df6c712b537156fcdb301e` data number · `num` 428 reference number · `refno` PRB078172506 common formula of materials · `name` AsF6 full material name · `fullname` beta-(BDA-TTP)2AsF6 shape · `shape` 3 structure · `str` BDA-TTP 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` 6.92 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` OTC428 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method. figure1 data file name · `f1_filename` OTC428.dat f2 data file name · `f2_filename` — title · `title` Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression year · `year` 2008 keyword · `keyword` — institute · `institute` Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan journal · `journal` Phys.Rev.B, 78(2008)172506 author · `author` Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi sample · `sample` — comments · `comments` —
(TMTSF)2ClO4Row 429 · TMTSF	Tc 1.2	Critical pressure, pcrit 0 GPa	1997 · PRL0792125 Method —
Inspect row 429: properties, remarks and source Thermal Conductivity of Superconducting (TMTSF)2ClO4: Evidence for a Nodeless Gap Phys.Rev.Lett., 79(1997)2125 Source remark: RRR=440. Tc defined by 0.5Rn. gap obtained by fitting the data of thermal conductivity to BRTmodel. gap has no nodes. Common name (raw) ClO4 Sample form Single crystal bulk (code 3) Energy gap at 0 K (raw) 4.6 Gap method Thermal conductivity (code 3) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 413–413; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6af874f6e0f00e7f5d71673d2852cbd3524ad7bbc186d60a7f73a4b770f57810` data number · `num` 429 reference number · `refno` PRL0792125 common formula of materials · `name` ClO4 full material name · `fullname` (TMTSF)2ClO4 shape · `shape` 3 structure · `str` TMTSF 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` 1.2 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 4.6 method of measuring energy gap · `gapmeth` 3 coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OTHC429 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` RRR=440. Tc defined by 0.5Rn. gap obtained by fitting the data of thermal conductivity to BRTmodel. gap has no nodes. figure1 data file name · `f1_filename` OTHC429.dat f2 data file name · `f2_filename` — title · `title` Thermal Conductivity of Superconducting (TMTSF)2ClO4: Evidence for a Nodeless Gap year · `year` 1997 keyword · `keyword` — institute · `institute` Laboratoire de Physique des Solides (CNRS), Universite Paris-Sud, 91405 Orsay, France journal · `journal` Phys.Rev.Lett., 79(1997)2125 author · `author` Stephane Belin,Kamran Behnia sample · `sample` — comments · `comments` —
kapa-(BEDT-TTF)2Cu[N(CN)2]BrRow 430 · BEDT-TTF	Tc 11.6	Critical pressure, pcrit 0 GPa	1990 · PRB0428686 Method —
Inspect row 430: properties, remarks and source Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor: kappa-(BEDT-TTF)2Cu[N(CN)2]Br Phys.Rev.B, 42(1990)8686 Source remark: 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. Common name (raw) Cu[N(CN)2]Br Sample form Single crystal bulk (code 3) −dHc2/dT at Tc (raw) 2.3 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 414–414; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `9abf0bce9ef33d27d49f7d200f2ffd73c7bc58c23cecb6482238cae5bcf474e4` data number · `num` 430 reference number · `refno` PRB0428686 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kapa-(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` 11.6 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 2.3 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` OHC430 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` OHC430.dat f2 data file name · `f2_filename` — title · `title` Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor: kappa-(BEDT-TTF)2Cu[N(CN)2]Br year · `year` 1990 keyword · `keyword` — institute · `institute` Argonne National Laboratory, Argonne, Illinois journal · `journal` Phys.Rev.B, 42(1990)8686 author · `author` 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 sample · `sample` — comments · `comments` —
kapa-(BEDT-TTF)2Cu[N(CN)2]BrRow 431 · BEDT-TTF	Tc 11.6	Critical pressure, pcrit 0 GPa	1995 · PRL0754122 Method —
Inspect row 431: properties, remarks and source 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 Phys.Rev.Lett., 75(1995)4122 Source remark: <13>Cu-NMR. Hc2//b obtained by extraporation assuming Korringa law. For H//ac, this assumption not valid. Common name (raw) Cu[N(CN)2]Br Sample form Single crystal bulk (code 3) Hc2 at 0 K (raw) 10 Coherence length at 0 K (raw) 60 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 415–415; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `2a86d561ef22bb2dc1f5615c8927716f0a1aaac7bb32ebc1336ec4235c211b7c` data number · `num` 431 reference number · `refno` PRL0754122 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kapa-(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` 11.6 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` 10 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 60 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` <13>Cu-NMR. Hc2//b obtained by extraporation assuming Korringa law. For H//ac, this assumption not valid. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` 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 year · `year` 1995 keyword · `keyword` — institute · `institute` — journal · `journal` Phys.Rev.Lett., 75(1995)4122 author · `author` H.Mayaffre,P.Wzietek,D.Jerome,C.Lenoir,P.Batail sample · `sample` — comments · `comments` —
(TMTSF)2ClO4Row 432 · TMTSF	Tc 1.221	Critical pressure, pcrit 0 GPa	1983 · JPC0163535 Method —
Inspect row 432: properties, remarks and source The magnetic field dependence of the specific heat in (TMTSF)2ClO4 J.Phys.C: Solid State Phys., 16(1983)3535 Source remark: (dC) = 21.6 mJ/mol.K. (dC/gammaTc) = 1.67. Thermodynamic Hc(0) = 44 Oe. lattice term of SP: beta = 11.5 mJ/mol.K4. SP(H) also measured. Common name (raw) ClO4 Sample form Single crystal bulk (code 3) Electronic specific heat coefficient (raw) 10.5 Debye temperature (raw) 213 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 416–416; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `b82debd3bc3bd26a628e7a0e325b46794297aaa8333b5d1c95e5680351f3215a` data number · `num` 432 reference number · `refno` JPC0163535 common formula of materials · `name` ClO4 full material name · `fullname` (TMTSF)2ClO4 shape · `shape` 3 structure · `str` TMTSF 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` 1.221 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=AM^(-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` 10.5 Debye temperature · `debyet` 213 Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OSP432 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` (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. figure1 data file name · `f1_filename` OSP432.dat f2 data file name · `f2_filename` — title · `title` The magnetic field dependence of the specific heat in (TMTSF)2ClO4 year · `year` 1983 keyword · `keyword` — institute · `institute` — journal · `journal` J.Phys.C: Solid State Phys., 16(1983)3535 author · `author` R Brusetti,P Garoche,K Bechgaard sample · `sample` — comments · `comments` —
beta-(meso-DMBEDT-TTF)2PF6Row 433 · DMBEDT-TTF	Tc 4.6 Maximum Tc 4.6	Critical pressure, pcrit 0.06 GPa At maximum Tc, pmax (raw) 0.06	2009 · PRB080092508 Method —
Inspect row 433: properties, remarks and source Superconductivity competitive with checkerboard-type charge ordering in the organic conductor beta-(meso-DMBEDT-TTF)2PF6 Phys.Rev.B, 80(2009)092508 Source remark: 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. Common name (raw) PF6 Sample form Single crystal bulk (code 3) dTc/dP at P = 0 (raw) -4 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 417–417; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `1b6339cafa584cae104e369d55ae6bea31aee17e856d80d4a449cb100058a852` data number · `num` 433 reference number · `refno` PRB080092508 common formula of materials · `name` PF6 full material name · `fullname` beta-(meso-DMBEDT-TTF)2PF6 shape · `shape` 3 structure · `str` DMBEDT-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` 4.6 maximum tc under pressure · `tcmax` 4.6 applied pressure for tcmax · `pmax` 0.06 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.06 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` -4 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` OTC433 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` 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. figure1 data file name · `f1_filename` OTC433.dat f2 data file name · `f2_filename` — title · `title` Superconductivity competitive with checkerboard-type charge ordering in the organic conductor beta-(meso-DMBEDT-TTF)2PF6 year · `year` 2009 keyword · `keyword` — institute · `institute` Institute for Solid State Physics, The University of Tokyo, Kashiwa 277-8581, Japan journal · `journal` Phys.Rev.B, 80(2009)092508 author · `author` 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 sample · `sample` — comments · `comments` —
kappa-[(BEDT-TTF)1-x(BMDT-TTF)x]2Cu(NCS)2Row 434 · BEDT-TTF	Tc 9.26	Critical pressure, pcrit 0 GPa	2009 · JPCS150052224 Method —
Inspect row 434: properties, remarks and source Disorder effect on superconductivity in organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 J.Phys.: Conf.Series, 150(2009)052224 Source remark: samples with (BMDT-TTF) impurity as a scattering center. scattering effect on Tc were measured. Common name (raw) Cu(NCS)2 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 418–418; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `7a29986a76b24cf057c2fb4d588e24585f7c2c73021f77c2c8264d641def5fa5` data number · `num` 434 reference number · `refno` JPCS150052224 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-[(BEDT-TTF)1-x(BMDT-TTF)x]2Cu(NCS)2 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` 9.26 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` OTC434 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` samples with (BMDT-TTF) impurity as a scattering center. scattering effect on Tc were measured. figure1 data file name · `f1_filename` OTC434.dat f2 data file name · `f2_filename` — title · `title` Disorder effect on superconductivity in organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 year · `year` 2009 keyword · `keyword` — institute · `institute` Institute for Materials Research, Tohoku University, 980-8577 Sendai, Japan journal · `journal` J.Phys.: Conf.Series, 150(2009)052224 author · `author` T. Sasaki,H. Oizumi,N. Yoneyama,N. Kobayashi sample · `sample` — comments · `comments` —
(Per)2[Au(mnt)]2Row 435 · Per	Tc 0.313 Maximum Tc 0.313	Critical pressure, pcrit 0.53 GPa At maximum Tc, pmax (raw) 0.53	2009 · EPL08527009 Method —
Inspect row 435: properties, remarks and source Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2] Europhys.Lett., 85(2009)27009 Source remark: (Per) = perylene. Hc2(0) = 49.4 mT at P = 5.3 kbar. Hc2 defined as R=0.9Rn. T<CDW> = 12 K. Common name (raw) [Au(mnt)]2 Sample form Single crystal bulk (code 3) Hc2 at 0 K (raw) 0.0494 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 419–419; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `1e3ab72cf089060dd6eee6d512d9dfe2e610d5961853475b81062af3ef5fa5ae` data number · `num` 435 reference number · `refno` EPL08527009 common formula of materials · `name` [Au(mnt)]2 full material name · `fullname` (Per)2[Au(mnt)]2 shape · `shape` 3 structure · `str` Per 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` 0.313 maximum tc under pressure · `tcmax` 0.313 applied pressure for tcmax · `pmax` 0.53 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.53 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` 0.0494 -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` OHC435 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` (Per) = perylene. Hc2(0) = 49.4 mT at P = 5.3 kbar. Hc2 defined as R=0.9Rn. T<CDW> = 12 K. figure1 data file name · `f1_filename` OHC435.dat f2 data file name · `f2_filename` — title · `title` Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2] year · `year` 2009 keyword · `keyword` — institute · `institute` Physics/NHMFL Florida State University - Tallahassee, FL 32310, USA journal · `journal` Europhys.Lett., 85(2009)27009 author · `author` D. Graf,J. S. Brooks,M. Almeida,J. C. Dias,S. Uji,T. Terashima,M. Kimata sample · `sample` — comments · `comments` —
beta'-(BEDT-TTF)2IBrClRow 436 · BEDT-TTF	Tc 8.5 Maximum Tc 8.5	Critical pressure, pcrit 8.6 GPa At maximum Tc, pmax (raw) 8.6	2009 · JPCS150052093 Method —
Inspect row 436: properties, remarks and source Superconductivity induced by extremely high pressures in organic Mott-insulator beta'-(BEDTTTF)2IBrCl J.Phys.: Conf.Series, 150(2009)052093 Source remark: 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) Common name (raw) IBrCl 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 420–420; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `3fdcf7103b3199f53a5e3522f3e33e67c30e6f59f296a32f81b4245112edffc0` data number · `num` 436 reference number · `refno` JPCS150052093 common formula of materials · `name` IBrCl full material name · `fullname` beta'-(BEDT-TTF)2IBrCl 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` 8.5 maximum tc under pressure · `tcmax` 8.5 applied pressure for tcmax · `pmax` 8.6 Critical pressure/GPa at which Tc can be observed · `pcrit` 8.6 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` 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) figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity induced by extremely high pressures in organic Mott-insulator beta'-(BEDTTTF)2IBrCl year · `year` 2009 keyword · `keyword` — institute · `institute` National High Magnetic Field Laboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA journal · `journal` J.Phys.: Conf.Series, 150(2009)052093 author · `author` M Kano,K Uchiyama,H Taniguchi,M Hedo,K Matsubayashi,Y Uwatoko sample · `sample` — comments · `comments` —
(TMTTF)2PF6Row 437 · TMTTF	Tc 2.27	Critical pressure, pcrit 4.4 GPa At maximum Tc, pmax (raw) 4.48	2009 · PHB4043246 Method —
Inspect row 437: properties, remarks and source Anisotropy of the upper critical field in ultrahigh-pressure-induced superconductor (TMTTF)2PF6 Physica B, 404(2009)3246 Source remark: Hc2 defined as Tc(on). Hc2 for H//a, H//b', H//c* were measured at P = 4.48 GPa. Common name (raw) PF6 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 421–421; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `81bd41f4a3ac969fd34591f3184c909f126284339965e29aa89a3e1323d6e588` data number · `num` 437 reference number · `refno` PHB4043246 common formula of materials · `name` PF6 full material name · `fullname` (TMTTF)2PF6 shape · `shape` 3 structure · `str` TMTTF 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` 2.27 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` 4.48 Critical pressure/GPa at which Tc can be observed · `pcrit` 4.4 tc measurement method · `tcmeth` — alpha in Tc=AM^(-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` OHC437 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 defined as Tc(on). Hc2 for H//a, H//b', H//c were measured at P = 4.48 GPa. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Anisotropy of the upper critical field in ultrahigh-pressure-induced superconductor (TMTTF)2PF6 year · `year` 2009 keyword · `keyword` — institute · `institute` National HigMagnetiFielLaboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA journal · `journal` Physica B, 404(2009)3246 author · `author` Mika Kano,Hatsumi Mori,Yoshiya Uwatoko,Stan Tozer sample · `sample` — comments · `comments` —
beta-(BEDT-TTF)2I3Row 438 · BEDT-TTF	Tc 1.5 Maximum Tc 9	Critical pressure, pcrit 0 GPa At maximum Tc, pmax (raw) 0.4	2010 · PHB405S262 Method —
Inspect row 438: properties, remarks and source Superconductivityof beta-type salts under uniaxial compression Physica B, 405(2010)S262 Source remark: donor stack (along c-axis). FIG shows uniaxial-P effect of Tc. 8K-phase stabilized by embedding crystal into epoxy. Common name (raw) I3 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 422–422; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `cc6920ed4f168010247c54ce01484fd851bf1c7e266a281bea0d73584b9871eb` data number · `num` 438 reference number · `refno` PHB405S262 common formula of materials · `name` I3 full material name · `fullname` beta-(BEDT-TTF)2I3 shape · `shape` — 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` 1.5 maximum tc under pressure · `tcmax` 9 applied pressure for tcmax · `pmax` 0.4 Critical pressure/GPa at which Tc can be observed · `pcrit` 0 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` OTC438 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` donor stack (along c-axis). FIG shows uniaxial-P effect of Tc. 8K-phase stabilized by embedding crystal into epoxy. figure1 data file name · `f1_filename` OTC438.dat f2 data file name · `f2_filename` — title · `title` Superconductivityof beta-type salts under uniaxial compression year · `year` 2010 keyword · `keyword` — institute · `institute` Department of Applied Physics, Nagoya University, Japan journal · `journal` Physica B, 405(2010)S262 author · `author` Hiroshi Ito,Tetsuo Ishihara,Masafumi Niwa,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Hideki Yamochi,Gunzi Saito sample · `sample` — comments · `comments` —

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-((ET)0.95(MT)0.05)2Cu(NCS)2Row 419 · BEDT-TTF

Tc: 7.9

Critical pressure, pcrit: 0 GPa

2007 · J076123705

Method —

Inspect row 419: properties, remarks and source

Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2

J.Phys.Soc.Jpn, 76(2007)123705

Source remark: impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence.

Common name (raw): Cu(NCS)2
Sample form: Not supplied
Coherence length at 0 K (raw): 66
Penetration depth at 0 K (raw): 0.465

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

All 49 original cells and provenance

Original physical lines 403–403; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6c347bcb83ca47678756778c1ed3fc38a4a47ca8a67f38fcc73ee9e3abe26d85

data number · num: 419
reference number · refno: J076123705
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-((ET)0.95(MT)0.05)2Cu(NCS)2
shape · shape: —
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: 7.9
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 66
penetration depth at 0 K for poly crystal · penet: 0.465
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: OHC418
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: impurity(MT-molecule) effect. slow cooled(0.2K/min) samples. [penet] from M-H curves using London model and d-wave dependence.
figure1 data file name · f1_filename: OHC418.dat
f2 data file name · f2_filename: —
title · title: Impurity Effect on Superconducting Properties in Molecular Substituted Organic Superconductor kappa-(ET)2Cu(NCS)2
year · year: 2007
keyword · keyword: —
institute · institute: Institute for Materials Research, Tohoku University, Sendai 980-8577
journal · journal: J.Phys.Soc.Jpn, 76(2007)123705
author · author: Naoki YONEYAMA,Takahiko SASAKI,Hajime OIZUMI,Norio KOBAYASHI
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 420 · BEDT-TTF

Tc: 9.2

Critical pressure, pcrit: 0 GPa

2004 · JPS0731290

Method —

Inspect row 420: properties, remarks and source

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)

J.Phys.Soc.Jpn, 73(2004)1290

Source remark: Tc not depends on cooling rate. [penet] by magnetization.

Common name (raw): Cu(NCS)2
Sample form: Not supplied
Penetration depth at 0 K (raw): 0.43

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

All 49 original cells and provenance

Original physical lines 404–404; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 86f761985e986b2b5f6908abddba779139d7325d32ef57348e06ace60c79fbfa

data number · num: 420
reference number · refno: JPS0731290
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
shape · shape: —
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: 9.2
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 0.43
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: OTC421
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Tc not depends on cooling rate. [penet] by magnetization.
figure1 data file name · f1_filename: OTC421.dat
f2 data file name · f2_filename: —
title · title: 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)
year · year: 2004
keyword · keyword: —
institute · institute: Institute for Materials Research, Tohoku University, Sendai 980-8577
journal · journal: J.Phys.Soc.Jpn, 73(2004)1290
author · author: Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 421 · BEDT-TTF

Tc: 11.7

Critical pressure, pcrit: 0 GPa

2004 · JPS0731290

Method —

Inspect row 421: properties, remarks and source

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)

J.Phys.Soc.Jpn, 73(2004)1290

Source remark: 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).

Common name (raw): Cu[N(CN)2]Br
Sample form: Not supplied
Penetration depth at 0 K (raw): 0.57

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

All 49 original cells and provenance

Original physical lines 405–405; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 916e13e1b22990b5362cf327f3f27060b20f44adda0e65ef49344313552e8cec

data number · num: 421
reference number · refno: JPS0731290
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: —
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: 11.7
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 0.57
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: 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).
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: 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)
year · year: 2004
keyword · keyword: —
institute · institute: Institute for Materials Research, Tohoku University, Sendai 980-8577
journal · journal: J.Phys.Soc.Jpn, 73(2004)1290
author · author: Naoki YONEYAMA,Akihiro HIGASHIHARA,Takahiko SASAKI,Tsutomu NOJIMA,Norio KOBAYASHI
sample · sample: —
comments · comments: —

(MDT-TS)(AuI2)0.441Row 422 · MDT-TS

Tc: 4.9
Maximum Tc: 4.9

Critical pressure, pcrit: 1.05 GPa
At maximum Tc, pmax (raw): 1.27

2008 · P077224506

Method —

Inspect row 422: properties, remarks and source

Antiferromagnetic ordering of the incommensurate organic superconductor (MDT-TS)(AuI2)0.441 with a high spin-flop field

Phys.Rev.B, 77(2008)224506

Source remark: 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.

Common name (raw): AuI2
Sample form: Not supplied
Néel temperature (raw): 50

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

All 49 original cells and provenance

Original physical lines 406–406; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: edecd9350428d9fa017838b44b6e4426a831c69298b8899c1caecf931eb587ae

data number · num: 422
reference number · refno: P077224506
common formula of materials · name: AuI2
full material name · fullname: (MDT-TS)(AuI2)0.441
shape · shape: —
structure · str: MDT-TS
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: 4.9
maximum tc under pressure · tcmax: 4.9
applied pressure for tcmax · pmax: 1.27
Critical pressure/GPa at which Tc can be observed · pcrit: 1.05
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: 50
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Antiferromagnetic ordering of the incommensurate organic superconductor (MDT-TS)(AuI2)0.441 with a high spin-flop field
year · year: 2008
keyword · keyword: —
institute · institute: Department of Organic and Polymeric Materials, Graduate School of Science and Engineering, Tokyo Institute of Technology, O-okayama, Meguro-ku, Tokyo 152-8552, Japan
journal · journal: Phys.Rev.B, 77(2008)224506
author · author: Tadashi Kawamoto,Yoshimasa Bando,Takehiko Mori,Takako Konoike,Yamaguchi Takahide,Taichi Terashima,Shinya Uji,Kazuo Takimiya,Tetsuo Otsubo
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 423 · BEDT-TTFSample label: organic

Tc: 10.5

Critical pressure, pcrit: 0 GPa

1994 · PR04912990

Method —

Inspect row 423: properties, remarks and source

Magnetic penetration depth and fluxon-line dynamics in the organic superconductor k-[BEDT-TTF]2Cu[NCS]2

Phys.Rev.B, 49(1994)12990

Source remark: [penet] shows London [penet] calculated from muon-SR result (0.877 micron-m).

Common name (raw): Cu(NCS)2
Sample form: Single crystal bulk (code 3)
Lattice a (raw): 16.248
Lattice b (raw): 8.44
Lattice c (raw): 13.124
Lattice β (raw): 110.3
Hc2 at 0 K (raw): 7
Coherence length at 0 K (raw): 70
Penetration depth at 0 K (raw): 0.768
GL parameter (source glpar) (raw): 125

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

All 49 original cells and provenance

Original physical lines 407–407; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 7cabdbde396ea587ccc203e26dc9ea06e1570e16468010685abd9838277d4cff

data number · num: 423
reference number · refno: PR04912990
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
shape · shape: 3
structure · str: BEDT-TTF
lattice constant a · lata: 16.248
lattice constant b · latb: 8.44
lattice constant c · latc: 13.124
lattice alpha · alpha: —
lattice beta · beta: 110.3
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 10.5
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 7
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 70
penetration depth at 0 K for poly crystal · penet: 0.768
Ginzburg-Landau order parameter · glpar: 125
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: [penet] shows London [penet] calculated from muon-SR result (0.877 micron-m).
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Magnetic penetration depth and fluxon-line dynamics in the organic superconductor k-[BEDT-TTF]2Cu[NCS]2
year · year: 1994
keyword · keyword: —
institute · institute: —
journal · journal: Phys.Rev.B, 49(1994)12990
author · author: A.T.Fiory,D.Li.Williams,D.R.Harshman,E.Koster,I.Shinkoda,M.L.Kaplan,R.C.Haddon,T.Pfiz
sample · sample: organic
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 424 · BEDT-TTFSample label: ORGANIC

Tc: 8.3

Critical pressure, pcrit: 0 GPa

1994 · PR05013603

Method —

Inspect row 424: properties, remarks and source

Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br

Phys.Rev.B.,50(1994) 13603

Source remark: surface impedance. For out-of-plane, [penet] = 40 um and [cohere] = 5 A.

Common name (raw): Cu(NCS)2
Sample form: Single crystal bulk (code 3)
Coherence length at 0 K (raw): 70
Penetration depth at 0 K (raw): 1.4

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

All 49 original cells and provenance

Original physical lines 408–408; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 5a5901c7673091cb90ec32d19b815c71a4368d9ebbfe44b3759cc5ceb2e8beb9

data number · num: 424
reference number · refno: PR05013603
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
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: 8.3
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 70
penetration depth at 0 K for poly crystal · penet: 1.4
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: surface impedance. For out-of-plane, [penet] = 40 um and [cohere] = 5 A.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br
year · year: 1994
keyword · keyword: —
institute · institute: —
journal · journal: Phys.Rev.B.,50(1994) 13603
author · author: G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein
sample · sample: ORGANIC
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 425 · BEDT-TTFSample label: ORGANIC

Tc: 11.3

Critical pressure, pcrit: 0 GPa

1994 · PR05013603

Method —

Inspect row 425: properties, remarks and source

Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br

Phys.Rev.B.,50(1994) 13603

Source remark: surface impedance. For out-of-plane, [penet] = 38 um and [cohere] = 6 A.

Common name (raw): Cu[N(CN)2]Br
Sample form: Not supplied
Coherence length at 0 K (raw): 37
Penetration depth at 0 K (raw): 1.5
Energy gap at 0 K (raw): 5
Gap method: Surface impedance (code 7)

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

All 49 original cells and provenance

Original physical lines 409–409; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 293c7b9fb4209f15233db5e127f74ca4fb8729d683e730965456d10b50deefd4

data number · num: 425
reference number · refno: PR05013603
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: —
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: 11.3
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 37
penetration depth at 0 K for poly crystal · penet: 1.5
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: 5
method of measuring energy gap · gapmeth: 7
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: surface impedance. For out-of-plane, [penet] = 38 um and [cohere] = 6 A.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Electrodynamics of the organic superconductors k-(BEDT-TTF)2Cu(NCS)2and k-(BEDT-TTF)2Cu[N(CN)2]Br
year · year: 1994
keyword · keyword: —
institute · institute: —
journal · journal: Phys.Rev.B.,50(1994) 13603
author · author: G.Gruner,H.H.Wang,J.M.Williams,K.D.Carlson,M.Dressel,O.Klein
sample · sample: ORGANIC
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 426 · BEDT-TTF

Tc: 8.3

Critical pressure, pcrit: 0 GPa

1993 · PR04711595

Method —

Inspect row 426: properties, remarks and source

Microwave surface impedance of kappa-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene: Evidence for unconventional superconductivity

Phys.Rev.B, 47(1993)11595

Source remark: surface impedance.

Common name (raw): Cu(NCS)2
Sample form: Single crystal bulk (code 3)
Penetration depth at 0 K (raw): 2

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

All 49 original cells and provenance

Original physical lines 410–410; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 9955797391059a044ead1848091972e69953e924d7c0e84bf9914627e0b4a0de

data number · num: 426
reference number · refno: PR04711595
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
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: 8.3
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 2
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: surface impedance.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Microwave surface impedance of kappa-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene: Evidence for unconventional superconductivity
year · year: 1993
keyword · keyword: —
institute · institute: —
journal · journal: Phys.Rev.B, 47(1993)11595
author · author: D.Achkir,M.Poirier,C.Bourbonnais,G.Quirion,C.Lenoir,D.Jerome
sample · sample: —
comments · comments: —

beta-(BDA-TTP)2SbF6Row 427 · BDA-TTP

Tc: 7.32

Critical pressure, pcrit: 0 GPa

2008 · PRB078172506

Method —

Inspect row 427: properties, remarks and source

Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression

Phys.Rev.B, 78(2008)172506

Source remark: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.

Common name (raw): SbF6
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 411–411; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 198249640426be9921506a85a0a618f169fc42675ff38678bb74a1427a6f2511

data number · num: 427
reference number · refno: PRB078172506
common formula of materials · name: SbF6
full material name · fullname: beta-(BDA-TTP)2SbF6
shape · shape: 3
structure · str: BDA-TTP
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: 7.32
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: OTC427
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.
figure1 data file name · f1_filename: OTC427.dat
f2 data file name · f2_filename: —
title · title: Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression
year · year: 2008
keyword · keyword: —
institute · institute: Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan
journal · journal: Phys.Rev.B, 78(2008)172506
author · author: Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi
sample · sample: —
comments · comments: —

beta-(BDA-TTP)2AsF6Row 428 · BDA-TTP

Tc: 6.92

Critical pressure, pcrit: 0 GPa

2008 · PRB078172506

Method —

Inspect row 428: properties, remarks and source

Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression

Phys.Rev.B, 78(2008)172506

Source remark: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.

Common name (raw): AsF6
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 412–412; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: be4373483b740c351f7921e4d6f1676d0e970940b5df6c712b537156fcdb301e

data number · num: 428
reference number · refno: PRB078172506
common formula of materials · name: AsF6
full material name · fullname: beta-(BDA-TTP)2AsF6
shape · shape: 3
structure · str: BDA-TTP
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: 6.92
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: OTC428
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: P-dependence of Tc measured for uniaxial pressure. stripe is perpendicular to a+c direction. sample made by electrochemical method.
figure1 data file name · f1_filename: OTC428.dat
f2 data file name · f2_filename: —
title · title: Roles of spin fluctuation and frustration in the superconductivity of beta-(BDA-TTP)2X (X=SbF6 , AsF6) under uniaxial compression
year · year: 2008
keyword · keyword: —
institute · institute: Department of Applied Physics, Nagoya University, Chikusa, Nagoya 464-8603, Japan
journal · journal: Phys.Rev.B, 78(2008)172506
author · author: Hiroshi Ito,Tetsuo Ishihara,Hisaaki Tanaka,Shin-ichi Kuroda,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Koichi Kikuchi
sample · sample: —
comments · comments: —

(TMTSF)2ClO4Row 429 · TMTSF

Tc: 1.2

Critical pressure, pcrit: 0 GPa

1997 · PRL0792125

Method —

Inspect row 429: properties, remarks and source

Thermal Conductivity of Superconducting (TMTSF)2ClO4: Evidence for a Nodeless Gap

Phys.Rev.Lett., 79(1997)2125

Source remark: RRR=440. Tc defined by 0.5Rn. gap obtained by fitting the data of thermal conductivity to BRTmodel. gap has no nodes.

Common name (raw): ClO4
Sample form: Single crystal bulk (code 3)
Energy gap at 0 K (raw): 4.6
Gap method: Thermal conductivity (code 3)

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

All 49 original cells and provenance

Original physical lines 413–413; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6af874f6e0f00e7f5d71673d2852cbd3524ad7bbc186d60a7f73a4b770f57810

data number · num: 429
reference number · refno: PRL0792125
common formula of materials · name: ClO4
full material name · fullname: (TMTSF)2ClO4
shape · shape: 3
structure · str: TMTSF
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: 1.2
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 4.6
method of measuring energy gap · gapmeth: 3
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OTHC429
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: RRR=440. Tc defined by 0.5Rn. gap obtained by fitting the data of thermal conductivity to BRTmodel. gap has no nodes.
figure1 data file name · f1_filename: OTHC429.dat
f2 data file name · f2_filename: —
title · title: Thermal Conductivity of Superconducting (TMTSF)2ClO4: Evidence for a Nodeless Gap
year · year: 1997
keyword · keyword: —
institute · institute: Laboratoire de Physique des Solides (CNRS), Universite Paris-Sud, 91405 Orsay, France
journal · journal: Phys.Rev.Lett., 79(1997)2125
author · author: Stephane Belin,Kamran Behnia
sample · sample: —
comments · comments: —

kapa-(BEDT-TTF)2Cu[N(CN)2]BrRow 430 · BEDT-TTF

Tc: 11.6

Critical pressure, pcrit: 0 GPa

1990 · PRB0428686

Method —

Inspect row 430: properties, remarks and source

Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor: kappa-(BEDT-TTF)2Cu[N(CN)2]Br

Phys.Rev.B, 42(1990)8686

Source remark: 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.

Common name (raw): Cu[N(CN)2]Br
Sample form: Single crystal bulk (code 3)
−dHc2/dT at Tc (raw): 2.3

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

All 49 original cells and provenance

Original physical lines 414–414; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 9abf0bce9ef33d27d49f7d200f2ffd73c7bc58c23cecb6482238cae5bcf474e4

data number · num: 430
reference number · refno: PRB0428686
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kapa-(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: 11.6
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 2.3
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: OHC430
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: OHC430.dat
f2 data file name · f2_filename: —
title · title: Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
year · year: 1990
keyword · keyword: —
institute · institute: Argonne National Laboratory, Argonne, Illinois
journal · journal: Phys.Rev.B, 42(1990)8686
author · author: 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
sample · sample: —
comments · comments: —

kapa-(BEDT-TTF)2Cu[N(CN)2]BrRow 431 · BEDT-TTF

Tc: 11.6

Critical pressure, pcrit: 0 GPa

1995 · PRL0754122

Method —

Inspect row 431: properties, remarks and source

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

Phys.Rev.Lett., 75(1995)4122

Source remark: <13>Cu-NMR. Hc2//b obtained by extraporation assuming Korringa law. For H//ac, this assumption not valid.

Common name (raw): Cu[N(CN)2]Br
Sample form: Single crystal bulk (code 3)
Hc2 at 0 K (raw): 10
Coherence length at 0 K (raw): 60

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All 49 original cells and provenance

Original physical lines 415–415; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 2a86d561ef22bb2dc1f5615c8927716f0a1aaac7bb32ebc1336ec4235c211b7c

data number · num: 431
reference number · refno: PRL0754122
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kapa-(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: 11.6
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 10
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 60
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: <13>Cu-NMR. Hc2//b obtained by extraporation assuming Korringa law. For H//ac, this assumption not valid.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: 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
year · year: 1995
keyword · keyword: —
institute · institute: —
journal · journal: Phys.Rev.Lett., 75(1995)4122
author · author: H.Mayaffre,P.Wzietek,D.Jerome,C.Lenoir,P.Batail
sample · sample: —
comments · comments: —

(TMTSF)2ClO4Row 432 · TMTSF

Tc: 1.221

Critical pressure, pcrit: 0 GPa

1983 · JPC0163535

Method —

Inspect row 432: properties, remarks and source

The magnetic field dependence of the specific heat in (TMTSF)2ClO4

J.Phys.C: Solid State Phys., 16(1983)3535

Source remark: (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.

Common name (raw): ClO4
Sample form: Single crystal bulk (code 3)
Electronic specific heat coefficient (raw): 10.5
Debye temperature (raw): 213

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All 49 original cells and provenance

Original physical lines 416–416; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: b82debd3bc3bd26a628e7a0e325b46794297aaa8333b5d1c95e5680351f3215a

data number · num: 432
reference number · refno: JPC0163535
common formula of materials · name: ClO4
full material name · fullname: (TMTSF)2ClO4
shape · shape: 3
structure · str: TMTSF
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: 1.221
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: 10.5
Debye temperature · debyet: 213
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OSP432
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: (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.
figure1 data file name · f1_filename: OSP432.dat
f2 data file name · f2_filename: —
title · title: The magnetic field dependence of the specific heat in (TMTSF)2ClO4
year · year: 1983
keyword · keyword: —
institute · institute: —
journal · journal: J.Phys.C: Solid State Phys., 16(1983)3535
author · author: R Brusetti,P Garoche,K Bechgaard
sample · sample: —
comments · comments: —

beta-(meso-DMBEDT-TTF)2PF6Row 433 · DMBEDT-TTF

Tc: 4.6
Maximum Tc: 4.6

Critical pressure, pcrit: 0.06 GPa
At maximum Tc, pmax (raw): 0.06

2009 · PRB080092508

Method —

Inspect row 433: properties, remarks and source

Superconductivity competitive with checkerboard-type charge ordering in the organic conductor beta-(meso-DMBEDT-TTF)2PF6

Phys.Rev.B, 80(2009)092508

Source remark: 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.

Common name (raw): PF6
Sample form: Single crystal bulk (code 3)
dTc/dP at P = 0 (raw): -4

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All 49 original cells and provenance

Original physical lines 417–417; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 1b6339cafa584cae104e369d55ae6bea31aee17e856d80d4a449cb100058a852

data number · num: 433
reference number · refno: PRB080092508
common formula of materials · name: PF6
full material name · fullname: beta-(meso-DMBEDT-TTF)2PF6
shape · shape: 3
structure · str: DMBEDT-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: 4.6
maximum tc under pressure · tcmax: 4.6
applied pressure for tcmax · pmax: 0.06
Critical pressure/GPa at which Tc can be observed · pcrit: 0.06
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: -4
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: OTC433
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: 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.
figure1 data file name · f1_filename: OTC433.dat
f2 data file name · f2_filename: —
title · title: Superconductivity competitive with checkerboard-type charge ordering in the organic conductor beta-(meso-DMBEDT-TTF)2PF6
year · year: 2009
keyword · keyword: —
institute · institute: Institute for Solid State Physics, The University of Tokyo, Kashiwa 277-8581, Japan
journal · journal: Phys.Rev.B, 80(2009)092508
author · author: 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
sample · sample: —
comments · comments: —

kappa-[(BEDT-TTF)1-x(BMDT-TTF)x]2Cu(NCS)2Row 434 · BEDT-TTF

Tc: 9.26

Critical pressure, pcrit: 0 GPa

2009 · JPCS150052224

Method —

Inspect row 434: properties, remarks and source

Disorder effect on superconductivity in organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2

J.Phys.: Conf.Series, 150(2009)052224

Source remark: samples with (BMDT-TTF) impurity as a scattering center. scattering effect on Tc were measured.

Common name (raw): Cu(NCS)2
Sample form: Single crystal bulk (code 3)

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All 49 original cells and provenance

Original physical lines 418–418; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 7a29986a76b24cf057c2fb4d588e24585f7c2c73021f77c2c8264d641def5fa5

data number · num: 434
reference number · refno: JPCS150052224
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-[(BEDT-TTF)1-x(BMDT-TTF)x]2Cu(NCS)2
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: 9.26
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: OTC434
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: samples with (BMDT-TTF) impurity as a scattering center. scattering effect on Tc were measured.
figure1 data file name · f1_filename: OTC434.dat
f2 data file name · f2_filename: —
title · title: Disorder effect on superconductivity in organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2
year · year: 2009
keyword · keyword: —
institute · institute: Institute for Materials Research, Tohoku University, 980-8577 Sendai, Japan
journal · journal: J.Phys.: Conf.Series, 150(2009)052224
author · author: T. Sasaki,H. Oizumi,N. Yoneyama,N. Kobayashi
sample · sample: —
comments · comments: —

(Per)2[Au(mnt)]2Row 435 · Per

Tc: 0.313
Maximum Tc: 0.313

Critical pressure, pcrit: 0.53 GPa
At maximum Tc, pmax (raw): 0.53

2009 · EPL08527009

Method —

Inspect row 435: properties, remarks and source

Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2]

Europhys.Lett., 85(2009)27009

Source remark: (Per) = perylene. Hc2(0) = 49.4 mT at P = 5.3 kbar. Hc2 defined as R=0.9Rn. T<CDW> = 12 K.

Common name (raw): [Au(mnt)]2
Sample form: Single crystal bulk (code 3)
Hc2 at 0 K (raw): 0.0494

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All 49 original cells and provenance

Original physical lines 419–419; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 1e3ab72cf089060dd6eee6d512d9dfe2e610d5961853475b81062af3ef5fa5ae

data number · num: 435
reference number · refno: EPL08527009
common formula of materials · name: [Au(mnt)]2
full material name · fullname: (Per)2[Au(mnt)]2
shape · shape: 3
structure · str: Per
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: 0.313
maximum tc under pressure · tcmax: 0.313
applied pressure for tcmax · pmax: 0.53
Critical pressure/GPa at which Tc can be observed · pcrit: 0.53
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: 0.0494
-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: OHC435
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: (Per) = perylene. Hc2(0) = 49.4 mT at P = 5.3 kbar. Hc2 defined as R=0.9Rn. T<CDW> = 12 K.
figure1 data file name · f1_filename: OHC435.dat
f2 data file name · f2_filename: —
title · title: Evolution of superconductivity from a charge-density-wave ground state in pressurized (Per)2[Au(mnt)2]
year · year: 2009
keyword · keyword: —
institute · institute: Physics/NHMFL Florida State University - Tallahassee, FL 32310, USA
journal · journal: Europhys.Lett., 85(2009)27009
author · author: D. Graf,J. S. Brooks,M. Almeida,J. C. Dias,S. Uji,T. Terashima,M. Kimata
sample · sample: —
comments · comments: —

beta'-(BEDT-TTF)2IBrClRow 436 · BEDT-TTF

Tc: 8.5
Maximum Tc: 8.5

Critical pressure, pcrit: 8.6 GPa
At maximum Tc, pmax (raw): 8.6

2009 · JPCS150052093

Method —

Inspect row 436: properties, remarks and source

Superconductivity induced by extremely high pressures in organic Mott-insulator beta'-(BEDTTTF)2IBrCl

J.Phys.: Conf.Series, 150(2009)052093

Source remark: 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)

Common name (raw): IBrCl
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 420–420; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 3fdcf7103b3199f53a5e3522f3e33e67c30e6f59f296a32f81b4245112edffc0

data number · num: 436
reference number · refno: JPCS150052093
common formula of materials · name: IBrCl
full material name · fullname: beta'-(BEDT-TTF)2IBrCl
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: 8.5
maximum tc under pressure · tcmax: 8.5
applied pressure for tcmax · pmax: 8.6
Critical pressure/GPa at which Tc can be observed · pcrit: 8.6
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: 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)
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity induced by extremely high pressures in organic Mott-insulator beta'-(BEDTTTF)2IBrCl
year · year: 2009
keyword · keyword: —
institute · institute: National High Magnetic Field Laboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA
journal · journal: J.Phys.: Conf.Series, 150(2009)052093
author · author: M Kano,K Uchiyama,H Taniguchi,M Hedo,K Matsubayashi,Y Uwatoko
sample · sample: —
comments · comments: —

(TMTTF)2PF6Row 437 · TMTTF

Tc: 2.27

Critical pressure, pcrit: 4.4 GPa
At maximum Tc, pmax (raw): 4.48

2009 · PHB4043246

Method —

Inspect row 437: properties, remarks and source

Anisotropy of the upper critical field in ultrahigh-pressure-induced superconductor (TMTTF)2PF6

Physica B, 404(2009)3246

Source remark: Hc2 defined as Tc(on). Hc2 for H//a, H//b', H//c* were measured at P = 4.48 GPa.

Common name (raw): PF6
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 421–421; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 81bd41f4a3ac969fd34591f3184c909f126284339965e29aa89a3e1323d6e588

data number · num: 437
reference number · refno: PHB4043246
common formula of materials · name: PF6
full material name · fullname: (TMTTF)2PF6
shape · shape: 3
structure · str: TMTTF
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: 2.27
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: 4.48
Critical pressure/GPa at which Tc can be observed · pcrit: 4.4
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: OHC437
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 defined as Tc(on). Hc2 for H//a, H//b', H//c* were measured at P = 4.48 GPa.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Anisotropy of the upper critical field in ultrahigh-pressure-induced superconductor (TMTTF)2PF6
year · year: 2009
keyword · keyword: —
institute · institute: National HigMagnetiFielLaboratory, 1800 E. Paul Dirac Dr. Tallahassee, FL 32310, USA
journal · journal: Physica B, 404(2009)3246
author · author: Mika Kano,Hatsumi Mori,Yoshiya Uwatoko,Stan Tozer
sample · sample: —
comments · comments: —

beta-(BEDT-TTF)2I3Row 438 · BEDT-TTF

Tc: 1.5
Maximum Tc: 9

Critical pressure, pcrit: 0 GPa
At maximum Tc, pmax (raw): 0.4

2010 · PHB405S262

Method —

Inspect row 438: properties, remarks and source

Superconductivityof beta-type salts under uniaxial compression

Physica B, 405(2010)S262

Source remark: donor stack (along c-axis). FIG shows uniaxial-P effect of Tc. 8K-phase stabilized by embedding crystal into epoxy.

Common name (raw): I3
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 422–422; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: cc6920ed4f168010247c54ce01484fd851bf1c7e266a281bea0d73584b9871eb

data number · num: 438
reference number · refno: PHB405S262
common formula of materials · name: I3
full material name · fullname: beta-(BEDT-TTF)2I3
shape · shape: —
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: 1.5
maximum tc under pressure · tcmax: 9
applied pressure for tcmax · pmax: 0.4
Critical pressure/GPa at which Tc can be observed · pcrit: 0
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: OTC438
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: donor stack (along c-axis). FIG shows uniaxial-P effect of Tc. 8K-phase stabilized by embedding crystal into epoxy.
figure1 data file name · f1_filename: OTC438.dat
f2 data file name · f2_filename: —
title · title: Superconductivityof beta-type salts under uniaxial compression
year · year: 2010
keyword · keyword: —
institute · institute: Department of Applied Physics, Nagoya University, Japan
journal · journal: Physica B, 405(2010)S262
author · author: Hiroshi Ito,Tetsuo Ishihara,Masafumi Niwa,Takeo Suzuki,Seiichiro Onari,Yukio Tanaka,Jun-ichi Yamada,Hideki Yamochi,Gunzi Saito
sample · sample: —
comments · comments: —