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 · 241–260 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
ramda-(BETS)2GaBr1.5Cl2.5Row 258 · BETS	Tc 9.7 Maximum Tc 9.7	Critical pressure, pcrit 0.1 GPa At maximum Tc, pmax (raw) 0.3	1997 · PR05608526 Method —
Inspect row 258: properties, remarks and source Electric and magnetic properties and phase diagram of a series of organic superconductors ramda-BETS2GaXzY4-z : BETS = bis(ethylenedithiotetraselenafulvalene; X,Y = F, Cl, Br; 0<z<2)] Phys.Rev.B, 56(1997)R8526 Source remark: P-induced SC Common name (raw) GaBr1.5Cl2.5 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 243–243; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `050219413e8296306a3ac82f5b1c8e079715d8c6c1e7c93a1318f809bd837d8a` data number · `num` 258 reference number · `refno` PR05608526 common formula of materials · `name` GaBr1.5Cl2.5 full material name · `fullname` ramda-(BETS)2GaBr1.5Cl2.5 shape · `shape` 3 structure · `str` BETS 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` 9.7 maximum tc under pressure · `tcmax` 9.7 applied pressure for tcmax · `pmax` 0.3 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.1 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` OTC258 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` P-induced SC figure1 data file name · `f1_filename` OTC258.dat f2 data file name · `f2_filename` — title · `title` Electric and magnetic properties and phase diagram of a series of organic superconductors ramda-BETS2GaXzY4-z : BETS = bis(ethylenedithiotetraselenafulvalene; X,Y = F, Cl, Br; 0<z<2)] year · `year` 1997 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Okazaki 444, Japan journal · `journal` Phys.Rev.B, 56(1997)R8526 author · `author` H.Kobayashi,H.Akutsu,E.Arai,H.Tanaka,A.Kobayashi sample · `sample` — comments · `comments` —
(MDT-TSF)(I3)0.422Row 259 · MDT-TSF	Tc 4.9	—	2006 · P073094513 Method —
Inspect row 259: properties, remarks and source Charge transfer degree and superconductivity of the incommensurate organic superconductor (MDT-TSF)(I3)0.422 Phys.Rev.B, 73(2006)094513 Source remark: Hc2 by extraporation to T=0K. corere//a = 261, //b = 166, //c = 31 A at T=1.6 K. lata = 4.013 A for I3-salt. Dingle temp. = 0.48K for gamma-orbit, =1.3K for delta-orbit. Common name (raw) I3 Sample form Single crystal bulk (code 3) Lattice a (raw) 4.013 Hc2 at 0 K (raw) 7.1 Coherence length at 0 K (raw) 261 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 244–244; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `14e909a49756d79fcd474bc20edc1ea1f41af07f59ceb2a58fe6c474989f677f` data number · `num` 259 reference number · `refno` P073094513 common formula of materials · `name` I3 full material name · `fullname` (MDT-TSF)(I3)0.422 shape · `shape` 3 structure · `str` MDT-TSF lattice constant a · `lata` 4.013 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` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` 7.1 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 261 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` OHC259 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 by extraporation to T=0K. corere//a = 261, //b = 166, //c = 31 A at T=1.6 K. lata = 4.013 A for I3-salt. Dingle temp. = 0.48K for gamma-orbit, =1.3K for delta-orbit. figure1 data file name · `f1_filename` OHC259.dat f2 data file name · `f2_filename` — title · `title` Charge transfer degree and superconductivity of the incommensurate organic superconductor (MDT-TSF)(I3)0.422 year · `year` 2006 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, 73(2006)094513 author · `author` T.Kawamoto,T.Mori,T.Konoike,K.Enomoto,T.Terashima,S.Uji,H.Kitagawa,K.Takimiya,T.Otsubo sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 260 · BEDT-TTF	Tc 11.5	Critical pressure, pcrit 0 GPa	2002 · P065144521 Method —
Inspect row 260: properties, remarks and source Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors Phys.Rev.B, 65(2002)144521 Source remark: (dTc/dP) is for hydrostatic pressure which estimated using uniaxial-P-values; dTc/dP = -12.6(b-), = -11.6 (a-), and = -1.2 (c-axis) K/GPa. from thermal expansion coeffic. Common name (raw) Cu[N(CN)2]Br Sample form Single crystal bulk (code 3) dTc/dP at P = 0 (raw) -25.8 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 245–245; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `2d4bb14111450db63f1a21fa6ad9643fe4331c8ab67e90a0cff2e19c5ec9ee70` data number · `num` 260 reference number · `refno` P065144521 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` 3 structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 11.5 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 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` -25.8 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` (dTc/dP) is for hydrostatic pressure which estimated using uniaxial-P-values; dTc/dP = -12.6(b-), = -11.6 (a-), and = -1.2 (c-axis) K/GPa. from thermal expansion coeffic. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors year · `year` 2002 keyword · `keyword` — institute · `institute` Max-Planck-Institut fur Chemische Physik fester Stoffe, D-01187 Dresden, Germany journal · `journal` Phys.Rev.B, 65(2002)144521 author · `author` J.Muller,M.Lang,F.Steglich,J.A.Schlueter,A.M.Kini,T.Sasaki sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 261 · BETS	Tc 4.8	Critical pressure, pcrit 0 GPa	2006 · PHC4400017 Method —
Inspect row 261: properties, remarks and source Superconductivity and pseudogap states studied by microwave conductivity measurements of ramda-(BEDT-TSF)2GaCl4 Physica C, 440(2006)17 Source remark: Hc2 measured by micrwave loss. cohere for a-c plane. Common name (raw) GaCl4 Sample form Single crystal bulk (code 3) Hc2 at 0 K (raw) 3 −dHc2/dT at Tc (raw) 0.82 Coherence length at 0 K (raw) 87 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 246–246; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `f92201aa9303186ce2e9ea85337516442b6f225e25cd143475899cb0ec45a59e` data number · `num` 261 reference number · `refno` PHC4400017 common formula of materials · `name` GaCl4 full material name · `fullname` ramda-(BETS)2GaCl4 shape · `shape` 3 structure · `str` BETS 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` 4.8 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` 3 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` 0.82 coherence length at 0 K for poly crystal · `cohere` 87 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` OHC261 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 measured by micrwave loss. cohere for a*-c plane. figure1 data file name · `f1_filename` OHC261.dat f2 data file name · `f2_filename` — title · `title` Superconductivity and pseudogap states studied by microwave conductivity measurements of ramda-(BEDT-TSF)2GaCl4 year · `year` 2006 keyword · `keyword` — institute · `institute` Physics Department, Graduate School of Science, Tohoku University, Sendai 980-0845, Japan journal · `journal` Physica C, 440(2006)17 author · `author` T.Suzuki,E.Negishi,H.Uozaki,H.Matsui,N.Toyota sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 262 · BETS	Tc 5	Critical pressure, pcrit 0 GPa	2001 · JP01308325 Method —
Inspect row 262: properties, remarks and source Superconducting properties and Fermi-surface topology of the quasi-two-dimensional organic superconductor ramda-(BETS)2GaCl4 (BETS = bis(ethylene-dithio)tetraselenafulvalene) J.Phys.:Condens.Matter, 13(2001)8325 Source remark: Hc2 measured for H//b. dHvA effect, magnetoresistance, effective mass were measured. penet measured by LC inductance. Common name (raw) GaCl4 Sample form Single crystal bulk (code 3) Coherence length at 0 K (raw) 14 Penetration depth at 0 K (raw) 150 GL parameter (source glpar) (raw) 107 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 247–247; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `12a80562fd40ddaa29bd7af5b85d0b199d408733255410dbe9158e3955f90468` data number · `num` 262 reference number · `refno` JP01308325 common formula of materials · `name` GaCl4 full material name · `fullname` ramda-(BETS)2GaCl4 shape · `shape` 3 structure · `str` BETS 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` 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=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` 14 penetration depth at 0 K for poly crystal · `penet` 150 Ginzburg-Landau order parameter · `glpar` 107 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` OHC262 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 measured for H//b*. dHvA effect, magnetoresistance, effective mass were measured. penet measured by LC inductance. figure1 data file name · `f1_filename` OHC262.dat f2 data file name · `f2_filename` — title · `title` Superconducting properties and Fermi-surface topology of the quasi-two-dimensional organic superconductor ramda-(BETS)2GaCl4 (BETS = bis(ethylene-dithio)tetraselenafulvalene) year · `year` 2001 keyword · `keyword` — institute · `institute` National High Magnetic Field Laboratory, Los Alamos National Laboratory, MS-E536, Los Alamos, NM 87545, USA journal · `journal` J.Phys.:Condens.Matter, 13(2001)8325 author · `author` C.Mielke,J.Singleton,Moon-Sun Nam,N.Harrison,C.C.Agosta,B.Fravel,L.K.Montgomery sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 263 · BETS	Tc 5	Critical pressure, pcrit 0 GPa	2001 · SYN1200771 Method —
Inspect row 263: properties, remarks and source In-plane anisotropy of the upper critical field of ramda-(BETS)2GaCl4 Synth.Metals, 120(2001)771 Source remark: Hc2 by resistive transition. cohere(out-of-plane) = 9 A from dHc2/dT. Common name (raw) GaCl4 Sample form Single crystal bulk (code 3) Coherence length at 0 K (raw) 143 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 248–248; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `d629c5414654448d58b62637e3502df6edbd66677abea4f4a1204b8aac1f573f` data number · `num` 263 reference number · `refno` SYN1200771 common formula of materials · `name` GaCl4 full material name · `fullname` ramda-(BETS)2GaCl4 shape · `shape` 3 structure · `str` BETS 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` 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` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 143 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` OHC263 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 by resistive transition. cohere(out-of-plane) = 9 A from dHc2/dT. figure1 data file name · `f1_filename` OHC263.dat f2 data file name · `f2_filename` — title · `title` In-plane anisotropy of the upper critical field of ramda-(BETS)2GaCl4 year · `year` 2001 keyword · `keyword` — institute · `institute` Department of Physics,Kyoto University,Kyoto,Japan journal · `journal` Synth.Metals, 120(2001)771 author · `author` T.Kawasaki,M.A.Tanatar,T.Ishiguro,H.Tanaka,A.Kobayashi,H.Kobayashi sample · `sample` — comments · `comments` —
beta''-(BEDO-TTF)3Cu2(NCS)3Row 264 · BEDO-TTF	Tc 1.06	Critical pressure, pcrit 0 GPa	1990 · INO0291599 Method —
Inspect row 264: properties, remarks and source The first ambient pressure organic superconductor containing oxygen in the donor molecule, beta<m>-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K Inorg.Chem., 29(1990)1599 Source remark: monoclinic sublattice. single crystals were prepared by electrocrystallization. Common name (raw) Cu2(NCS)3 Sample form Not supplied Lattice a (raw) 4.237 Lattice b (raw) 33.481 Lattice c (raw) 5.273 Lattice β (raw) 97.94 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 249–249; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `0cd5ee60e83a75d33e11723285380a21a72cafbe64c4eb8cf3d7e06db12555e5` data number · `num` 264 reference number · `refno` INO0291599 common formula of materials · `name` Cu2(NCS)3 full material name · `fullname` beta''-(BEDO-TTF)3Cu2(NCS)3 shape · `shape` — structure · `str` BEDO-TTF lattice constant a · `lata` 4.237 lattice constant b · `latb` 33.481 lattice constant c · `latc` 5.273 lattice alpha · `alpha` — lattice beta · `beta` 97.94 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 1.06 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` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` monoclinic sublattice. single crystals were prepared by electrocrystallization. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` The first ambient pressure organic superconductor containing oxygen in the donor molecule, beta<m>-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K year · `year` 1990 keyword · `keyword` — institute · `institute` — journal · `journal` Inorg.Chem., 29(1990)1599 author · `author` M.A.Beno,H.H.Wang,A.M.Kini,K.D.Carlson,U.Geiser,W.K.Kwok,J.E.Thompson,J.M.Williams,J.Ren,M.H.Whangbo sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 265 · BEDT-TTF	Tc 12.5 Maximum Tc 12.5	Critical pressure, pcrit 0.03 GPa At maximum Tc, pmax (raw) 0.03	1990 · INO0293272 Method —
Inspect row 265: properties, remarks and source From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, kappa-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K) Inorg.Chem., 29(1990)3274 Source remark: space-G = Pnma. semicon-semicon transition at 42K. not SC down to 0.6K under ambient P. Common name (raw) Cu[N(CN)2]Cl Sample form Not supplied Lattice a (raw) 12.977 Lattice b (raw) 29.979 Lattice c (raw) 8.48 dTc/dP at P = 0 (raw) -34 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 250–250; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `8240e3811e8d8f44160e158698b6e5246190888d34b5ac123dd282958138824b` data number · `num` 265 reference number · `refno` INO0293272 common formula of materials · `name` Cu[N(CN)2]Cl full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Cl shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` 12.977 lattice constant b · `latb` 29.979 lattice constant c · `latc` 8.48 lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 12.5 maximum tc under pressure · `tcmax` 12.5 applied pressure for tcmax · `pmax` 0.03 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.03 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` -34 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` space-G = Pnma. semicon-semicon transition at 42K. not SC down to 0.6K under ambient P. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, kappa-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K) year · `year` 1990 keyword · `keyword` — institute · `institute` — journal · `journal` Inorg.Chem., 29(1990)3274 author · `author` J.M.Williams,A.M.Kini,H.H.Wang,K.D.Carlson,U.Geiser,L.K.Montgomery,G.J.Pyrka,D.M.Watkins,J.M.Kommers,S.J.Boryschuk,A.V.Strieby Crouch,W.K.Kwok,J.E..Schirber,D.L.Overmyer,D.Jung,M.H.Whangbo sample · `sample` — comments · `comments` —
(BEDO-TTF)2ReO4:(H2O)Row 266 · BEDO-TTF	Tc 0.9	Critical pressure, pcrit 0 GPa	1991 · SSC0800191 Method —
Inspect row 266: properties, remarks and source (BEDO-TTF)2REO4(H2O): A NEW ORGANIC SUPERCONDUCTOR+ SOLID STATE COMMUN.,80(1991)191 Source remark: monoclinic phase. Tc by susceptibility. Resistive Tc(on) = 2.5 K. Three phase transitions at 213K, 90K, 35K. Common name (raw) ReO4:(H2O) Sample form Not supplied Lattice a (raw) 12.16 Lattice b (raw) 34.05 Lattice c (raw) 8.091 Lattice β (raw) 123.44 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 251–251; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `8e3a4b3fb289fc693c743c756efa38daa35f06ede7131d0545f375ea2df55dcf` data number · `num` 266 reference number · `refno` SSC0800191 common formula of materials · `name` ReO4:(H2O) full material name · `fullname` (BEDO-TTF)2ReO4:(H2O) shape · `shape` — structure · `str` BEDO-TTF lattice constant a · `lata` 12.16 lattice constant b · `latb` 34.05 lattice constant c · `latc` 8.091 lattice alpha · `alpha` — lattice beta · `beta` 123.44 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0.9 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` — 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` monoclinic phase. Tc by susceptibility. Resistive Tc(on) = 2.5 K. Three phase transitions at 213K, 90K, 35K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` (BEDO-TTF)2REO4(H2O): A NEW ORGANIC SUPERCONDUCTOR+ year · `year` 1991 keyword · `keyword` — institute · `institute` 3.PHYSIKALISCHES INSTITUT DER UNIVERSITAT STUTTGART,PFAFFENWALDRING 57,7000 STUTTGART 80,GERMANY journal · `journal` SOLID STATE COMMUN.,80(1991)191 author · `author` B.NEBER,D.SCHWEITZER,H.J.KELLER,H.W.HELBERG,I.HEINEN,K.WINZER,S.KAHLICH,SONG EN LAN sample · `sample` — comments · `comments` —
beta'-Me4Sb[Pd(dmit)2]2Row 267 · Pd(dmit)2	Tc 8.4 Maximum Tc 8.4	Critical pressure, pcrit 0.4 GPa At maximum Tc, pmax (raw) 0.45	2005 · JPS0740412 Method —
Inspect row 267: properties, remarks and source Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate) J.Phys.Soc.Jpn, 74(2005)412 Source remark: Me=CH3. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for hydrostatic-P (upto 15 kbar) and c-axis pressure. Common name (raw) Me4Sb 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 252–252; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `06be3913760424965f529a61c277bf41bde52df1d2b59c757d8d39338dbd2a1e` data number · `num` 267 reference number · `refno` JPS0740412 common formula of materials · `name` Me4Sb full material name · `fullname` beta'-Me4Sb[Pd(dmit)2]2 shape · `shape` — structure · `str` Pd(dmit)2 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` 8.4 maximum tc under pressure · `tcmax` 8.4 applied pressure for tcmax · `pmax` 0.45 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.4 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` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Me=CH3. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for hydrostatic-P (upto 15 kbar) and c*-axis pressure. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate) year · `year` 2005 keyword · `keyword` — institute · `institute` Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan journal · `journal` J.Phys.Soc.Jpn, 74(2005)412 author · `author` A.Tajima,A.Nakao,R.Kato sample · `sample` — comments · `comments` —
beta'-Me2Et2P[Pd(dmit)2]2Row 268 · Pd(dmit)2	Tc 6.1 Maximum Tc 6.1	Critical pressure, pcrit 0.4 GPa At maximum Tc, pmax (raw) 0.45	2005 · JPS0740412 Method —
Inspect row 268: properties, remarks and source Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate) J.Phys.Soc.Jpn, 74(2005)412 Source remark: Me=CH3. Et=C2H5. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for a-axis pressure. Common name (raw) Me2Et2P 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 253–253; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `4defc10e585aa66aa7a9fcda86e3d63a78ab8641c7e4910e367a1fd62001af77` data number · `num` 268 reference number · `refno` JPS0740412 common formula of materials · `name` Me2Et2P full material name · `fullname` beta'-Me2Et2P[Pd(dmit)2]2 shape · `shape` — structure · `str` Pd(dmit)2 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` 6.1 maximum tc under pressure · `tcmax` 6.1 applied pressure for tcmax · `pmax` 0.45 Critical pressure/GPa at which Tc can be observed · `pcrit` 0.4 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` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Me=CH3. Et=C2H5. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for a-axis pressure. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate) year · `year` 2005 keyword · `keyword` — institute · `institute` Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan journal · `journal` J.Phys.Soc.Jpn, 74(2005)412 author · `author` A.Tajima,A.Nakao,R.Kato sample · `sample` — comments · `comments` —
beta'-Me4As[Pd(dmit)2]2Row 269 · Pd(dmit)2	Tc 4	Critical pressure, pcrit 0.7 GPa	2002 · P066020508 Method —
Inspect row 269: properties, remarks and source Uniaxial strain effect in a strongly correlated two-dimensional system beta'-(CH3)4As[Pd(dmit)2]2 Phys.Rev.B, 66(2002)020508R Source remark: Me=CH3. SC for b-axis pressure (7 < P < 10 kbar). not SC for a- and c-axis pressure. Common name (raw) Me4As 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 254–254; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `bb8d4035c1cd9a25f87968ecdbb072c80c49a1b3662b4f0f6deb26343b028135` data number · `num` 269 reference number · `refno` P066020508 common formula of materials · `name` Me4As full material name · `fullname` beta'-Me4As[Pd(dmit)2]2 shape · `shape` — structure · `str` Pd(dmit)2 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 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0.7 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` Me=CH3. SC for b-axis pressure (7 < P < 10 kbar). not SC for a- and c-axis pressure. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Uniaxial strain effect in a strongly correlated two-dimensional system beta'-(CH3)4As[Pd(dmit)2]2 year · `year` 2002 keyword · `keyword` — institute · `institute` Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan journal · `journal` Phys.Rev.B, 66(2002)020508R author · `author` R.Kato,N.Tajima,M.Tamura,J.Yamaura sample · `sample` — comments · `comments` —
beta'-Me2Et2P[Pd(dmit)2]2Row 270 · Pd(dmit)2	Tc 4	Critical pressure, pcrit 0.69 GPa	1998 · SSC1050561 Method —
Inspect row 270: properties, remarks and source A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate) Solid State Commun., 105(1998)561 Source remark: Me=CH3. Et=C2H5. SC-region: 6.9 =< P =< 10.4 kbar. Tc=1.8 K at P=10.4 kbar. R(H,T) measured at P=6.9 kbar. two dimensionality (r/B) = 0.82. Common name (raw) Me2Et2P Sample form Not supplied dTc/dP at P = 0 (raw) -6 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 255–255; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `9ab074f0144b1d79dac24ee87ba3a3d6a2a7822bfbf5b10c5ade7c1de806fc2d` data number · `num` 270 reference number · `refno` SSC1050561 common formula of materials · `name` Me2Et2P full material name · `fullname` beta'-Me2Et2P[Pd(dmit)2]2 shape · `shape` — structure · `str` Pd(dmit)2 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 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0.69 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` -6 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` Me=CH3. Et=C2H5. SC-region: 6.9 =< P =< 10.4 kbar. Tc=1.8 K at P=10.4 kbar. R(H,T) measured at P=6.9 kbar. two dimensionality (r/B) = 0.82. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate) year · `year` 1998 keyword · `keyword` — institute · `institute` ISSP, The University of Tokyo,Tokyo,Japan journal · `journal` Solid State Commun., 105(1998)561 author · `author` R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima sample · `sample` — comments · `comments` —
beta'-Me2Et2Sb[Pd(dmit)2]2Row 271 · Pd(dmit)2	—	—	1998 · SSC1050561 Method —
Inspect row 271: properties, remarks and source A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate) Solid State Commun., 105(1998)561 Source remark: Me=CH3. Et=C2H5. not SC upto 10.4 kbar. two dimensionality (r/B) = 0.96. Common name (raw) Me2Et2Sb 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 256–256; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `c25477a08b59d5d70712beec02fdd93711a9c34ca288874fcd5111efde193a4b` data number · `num` 271 reference number · `refno` SSC1050561 common formula of materials · `name` Me2Et2Sb full material name · `fullname` beta'-Me2Et2Sb[Pd(dmit)2]2 shape · `shape` — structure · `str` Pd(dmit)2 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` — maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Me=CH3. Et=C2H5. not SC upto 10.4 kbar. two dimensionality (r/B) = 0.96. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate) year · `year` 1998 keyword · `keyword` — institute · `institute` ISSP, The University of Tokyo,Tokyo,Japan journal · `journal` Solid State Commun., 105(1998)561 author · `author` R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima sample · `sample` — comments · `comments` —
beta-(EDT-TTF)4Hg2.9I8Row 272 · EDT-TTF	Tc 8.1	Critical pressure, pcrit 0 GPa	2004 · SYN1400151 Method —
Inspect row 272: properties, remarks and source New ambient pressure organic superconductor with Tc = 8.1 K based on unsymmetrical donor molecule, ethylenedithiotetrathiafulvalene: (EDT-TTF)4Hg3-zI8, z=0.1-0.2 Synth.Metals, 140(2004)151 Source remark: COHERE(0) estimated from COHERE(1.43K)//=126A. nCOHERE(0)=22A from nCOHERE(1.43K)=25A. stoichiometry determined by EPMA. Common name (raw) Hg2.9I8 Sample form Not supplied Coherence length at 0 K (raw) 114 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 257–257; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `fd6bdd8a4c6798225d117f0c826efc716711f58877eb1d8bb484baf7adcb355a` data number · `num` 272 reference number · `refno` SYN1400151 common formula of materials · `name` Hg2.9I8 full material name · `fullname` beta-(EDT-TTF)4Hg2.9I8 shape · `shape` — structure · `str` EDT-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` 8.1 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` 114 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` OHC272 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` COHERE(0) estimated from COHERE(1.43K)//=126A. nCOHERE(0)=22A from nCOHERE(1.43K)=25A. stoichiometry determined by EPMA. figure1 data file name · `f1_filename` OHC272.dat f2 data file name · `f2_filename` — title · `title` New ambient pressure organic superconductor with Tc = 8.1 K based on unsymmetrical donor molecule, ethylenedithiotetrathiafulvalene: (EDT-TTF)4Hg3-zI8, z=0.1-0.2 year · `year` 2004 keyword · `keyword` — institute · `institute` Institute of Problems of Chemical Physics, Russian Academy of Science, Chernogolovka 142432, MD, Russia journal · `journal` Synth.Metals, 140(2004)151 author · `author` E.I.Zhilyaeva,S.A.Torunova,R.N.Lyubovskaya,G.A.Mousdis,G.C.Papavassiliou,J.A.A.J.Perenboom,S.I.Pesotskii,R.B.Lyubovskii sample · `sample` — comments · `comments` —
kappa-(BETS)2FeCl4Row 273 · BETS	Tc 0.1	Critical pressure, pcrit 0 GPa	2001 · CEM1590407 Method —
Inspect row 273: properties, remarks and source Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions J.Solid State Chem., 159(2001)407 Source remark: AF comfirmed by SP-heat. AF easy axis = a-axis. Common name (raw) FeCl4 Sample form Not supplied Néel temperature (raw) 0.45 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 258–258; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `c4b0cf85de8a6a2611be618171a51261fb820246c8efa97eb1d444eb802679d3` data number · `num` 273 reference number · `refno` CEM1590407 common formula of materials · `name` FeCl4 full material name · `fullname` kappa-(BETS)2FeCl4 shape · `shape` — structure · `str` BETS 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` 0.1 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` 0.45 figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` AF comfirmed by SP-heat. AF easy axis = a-axis. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions year · `year` 2001 keyword · `keyword` — institute · `institute` Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan journal · `journal` J.Solid State Chem., 159(2001)407 author · `author` T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi sample · `sample` — comments · `comments` —
kappa-(BETS)2FeBr4Row 274 · BETS	Tc 1	Critical pressure, pcrit 0 GPa	2001 · CEM1590407 Method —
Inspect row 274: properties, remarks and source Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions J.Solid State Chem., 159(2001)407 Source remark: oriented crystal Common name (raw) 4-Feb Sample form Not supplied Néel temperature (raw) 2.5 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 259–259; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6f215a1cb31f4b2c890a8931980e99665303041c4b4a9f516c548f36aed50943` data number · `num` 274 reference number · `refno` CEM1590407 common formula of materials · `name` 4-Feb full material name · `fullname` kappa-(BETS)2FeBr4 shape · `shape` — structure · `str` BETS 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 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` 2.5 figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` oriented crystal figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions year · `year` 2001 keyword · `keyword` — institute · `institute` Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan journal · `journal` J.Solid State Chem., 159(2001)407 author · `author` T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi sample · `sample` — comments · `comments` —
(DMET)2Au(CN)2Row 275 · DMET	Tc 0.8	Critical pressure, pcrit 0.5 GPa	1987 · CHL0870931 Method —
Inspect row 275: properties, remarks and source New organic superconductor, (DMET)2Au(CN)2 Chem.Lett., (1987)931 Source remark: M-I transition at 25K. Common name (raw) Au(CN)2 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 260–260; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `febb124458d8cbacb873f8c7891daef9b4da689a12aa32133f94de8fe1f044db` data number · `num` 275 reference number · `refno` CHL0870931 common formula of materials · `name` Au(CN)2 full material name · `fullname` (DMET)2Au(CN)2 shape · `shape` — structure · `str` DMET 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` 0.8 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0.5 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` M-I transition at 25K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New organic superconductor, (DMET)2Au(CN)2 year · `year` 1987 keyword · `keyword` — institute · `institute` — journal · `journal` Chem.Lett., (1987)931 author · `author` K.Kikuchi,M.Kikuchi,T.Namiki,K.Saito,I.Ikemoto,K.Murata,T.Ishiguro,K.Kobayashi sample · `sample` — comments · `comments` —
kappa-(BETS)2GaBr4Row 276 · BETS	Tc 1	Critical pressure, pcrit 0 GPa	2000 · JMC0100245 Method —
Inspect row 276: properties, remarks and source A new kappa-type organic superconductor based on BETS molecules, kappa- (BETS)2GaBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene] J.Mater.Chem., 10(2000)245 Source remark: Tc=0.5 - 1.0 K. Tc(on) = 1.3 K. Space-G = Pnma Common name (raw) GaBr4 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 261–261; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `d571a56b7076fc5371d6377d1c487dc756e6f2b856e0d5954f92b3112e97570e` data number · `num` 276 reference number · `refno` JMC0100245 common formula of materials · `name` GaBr4 full material name · `fullname` kappa-(BETS)2GaBr4 shape · `shape` — structure · `str` BETS 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 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` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Tc=0.5 - 1.0 K. Tc(on) = 1.3 K. Space-G = Pnma figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` A new kappa-type organic superconductor based on BETS molecules, kappa- (BETS)2GaBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene] year · `year` 2000 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Myodaiji-cho, Okazaki 444-8585, Japan journal · `journal` J.Mater.Chem., 10(2000)245 author · `author` H.Tanaka,E.Ojima,H.Fujiwara,Y.Nakazawa,H.Kobayashi,A.Kobayashi sample · `sample` — comments · `comments` —
beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhNO2Row 277 · BEDT-TTF	Tc 6.2	Critical pressure, pcrit 0 GPa	2001 · JMC0112095 Method —
Inspect row 277: properties, remarks and source New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene) J.Mater.Chem., 11(2001)2095 Source remark: space-G = C2/c. Curie-C = 3.877 emu/mole. Structure parameters are at 120 K. Common name (raw) [(H3O)Fe(C2O4)3]:PhNO2 Sample form Not supplied Lattice a (raw) 10.2732 Lattice b (raw) 19.9494 Lattice c (raw) 35.0304 Lattice β (raw) 92.969 Curie temperature (raw) -0.16 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 262–262; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `42a7f4e4ce52638c6b8313510940d36801176afeaa052cd3594faec15f0d33c6` data number · `num` 277 reference number · `refno` JMC0112095 common formula of materials · `name` [(H3O)Fe(C2O4)3]:PhNO2 full material name · `fullname` beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhNO2 shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` 10.2732 lattice constant b · `latb` 19.9494 lattice constant c · `latc` 35.0304 lattice alpha · `alpha` — lattice beta · `beta` 92.969 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 6.2 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` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` -0.16 Neel temperature · `neelt` — figure1 file name · `fig1` — figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` space-G = C2/c. Curie-C = 3.877 emu/mole. Structure parameters are at 120 K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene) year · `year` 2001 keyword · `keyword` — institute · `institute` Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK journal · `journal` J.Mater.Chem., 11(2001)2095 author · `author` S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs 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

ramda-(BETS)2GaBr1.5Cl2.5Row 258 · BETS

Tc: 9.7
Maximum Tc: 9.7

Critical pressure, pcrit: 0.1 GPa
At maximum Tc, pmax (raw): 0.3

1997 · PR05608526

Method —

Inspect row 258: properties, remarks and source

Electric and magnetic properties and phase diagram of a series of organic superconductors ramda-BETS2GaXzY4-z : BETS = bis(ethylenedithiotetraselenafulvalene; X,Y = F, Cl, Br; 0<z<2)]

Phys.Rev.B, 56(1997)R8526

Source remark: P-induced SC

Common name (raw): GaBr1.5Cl2.5
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 243–243; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 050219413e8296306a3ac82f5b1c8e079715d8c6c1e7c93a1318f809bd837d8a

data number · num: 258
reference number · refno: PR05608526
common formula of materials · name: GaBr1.5Cl2.5
full material name · fullname: ramda-(BETS)2GaBr1.5Cl2.5
shape · shape: 3
structure · str: BETS
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: 9.7
maximum tc under pressure · tcmax: 9.7
applied pressure for tcmax · pmax: 0.3
Critical pressure/GPa at which Tc can be observed · pcrit: 0.1
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: OTC258
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: P-induced SC
figure1 data file name · f1_filename: OTC258.dat
f2 data file name · f2_filename: —
title · title: Electric and magnetic properties and phase diagram of a series of organic superconductors ramda-BETS2GaXzY4-z : BETS = bis(ethylenedithiotetraselenafulvalene; X,Y = F, Cl, Br; 0<z<2)]
year · year: 1997
keyword · keyword: —
institute · institute: Institute for Molecular Science, Okazaki 444, Japan
journal · journal: Phys.Rev.B, 56(1997)R8526
author · author: H.Kobayashi,H.Akutsu,E.Arai,H.Tanaka,A.Kobayashi
sample · sample: —
comments · comments: —

(MDT-TSF)(I3)0.422Row 259 · MDT-TSF

Tc: 4.9

—

2006 · P073094513

Method —

Inspect row 259: properties, remarks and source

Charge transfer degree and superconductivity of the incommensurate organic superconductor (MDT-TSF)(I3)0.422

Phys.Rev.B, 73(2006)094513

Source remark: Hc2 by extraporation to T=0K. corere//a = 261, //b = 166, //c = 31 A at T=1.6 K. lata = 4.013 A for I3-salt. Dingle temp. = 0.48K for gamma-orbit, =1.3K for delta-orbit.

Common name (raw): I3
Sample form: Single crystal bulk (code 3)
Lattice a (raw): 4.013
Hc2 at 0 K (raw): 7.1
Coherence length at 0 K (raw): 261

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

All 49 original cells and provenance

Original physical lines 244–244; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 14e909a49756d79fcd474bc20edc1ea1f41af07f59ceb2a58fe6c474989f677f

data number · num: 259
reference number · refno: P073094513
common formula of materials · name: I3
full material name · fullname: (MDT-TSF)(I3)0.422
shape · shape: 3
structure · str: MDT-TSF
lattice constant a · lata: 4.013
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: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: 7.1
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 261
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: OHC259
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 by extraporation to T=0K. corere//a = 261, //b = 166, //c = 31 A at T=1.6 K. lata = 4.013 A for I3-salt. Dingle temp. = 0.48K for gamma-orbit, =1.3K for delta-orbit.
figure1 data file name · f1_filename: OHC259.dat
f2 data file name · f2_filename: —
title · title: Charge transfer degree and superconductivity of the incommensurate organic superconductor (MDT-TSF)(I3)0.422
year · year: 2006
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, 73(2006)094513
author · author: T.Kawamoto,T.Mori,T.Konoike,K.Enomoto,T.Terashima,S.Uji,H.Kitagawa,K.Takimiya,T.Otsubo
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 260 · BEDT-TTF

Tc: 11.5

Critical pressure, pcrit: 0 GPa

2002 · P065144521

Method —

Inspect row 260: properties, remarks and source

Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors

Phys.Rev.B, 65(2002)144521

Source remark: (dTc/dP) is for hydrostatic pressure which estimated using uniaxial-P-values; dTc/dP = -12.6(b-), = -11.6 (a-), and = -1.2 (c-axis) K/GPa. from thermal expansion coeffic.

Common name (raw): Cu[N(CN)2]Br
Sample form: Single crystal bulk (code 3)
dTc/dP at P = 0 (raw): -25.8

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

All 49 original cells and provenance

Original physical lines 245–245; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 2d4bb14111450db63f1a21fa6ad9643fe4331c8ab67e90a0cff2e19c5ec9ee70

data number · num: 260
reference number · refno: P065144521
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: 3
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 11.5
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 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: -25.8
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: (dTc/dP) is for hydrostatic pressure which estimated using uniaxial-P-values; dTc/dP = -12.6(b-), = -11.6 (a-), and = -1.2 (c-axis) K/GPa. from thermal expansion coeffic.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors
year · year: 2002
keyword · keyword: —
institute · institute: Max-Planck-Institut fur Chemische Physik fester Stoffe, D-01187 Dresden, Germany
journal · journal: Phys.Rev.B, 65(2002)144521
author · author: J.Muller,M.Lang,F.Steglich,J.A.Schlueter,A.M.Kini,T.Sasaki
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 261 · BETS

Tc: 4.8

Critical pressure, pcrit: 0 GPa

2006 · PHC4400017

Method —

Inspect row 261: properties, remarks and source

Superconductivity and pseudogap states studied by microwave conductivity measurements of ramda-(BEDT-TSF)2GaCl4

Physica C, 440(2006)17

Source remark: Hc2 measured by micrwave loss. cohere for a*-c plane.

Common name (raw): GaCl4
Sample form: Single crystal bulk (code 3)
Hc2 at 0 K (raw): 3
−dHc2/dT at Tc (raw): 0.82
Coherence length at 0 K (raw): 87

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All 49 original cells and provenance

Original physical lines 246–246; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: f92201aa9303186ce2e9ea85337516442b6f225e25cd143475899cb0ec45a59e

data number · num: 261
reference number · refno: PHC4400017
common formula of materials · name: GaCl4
full material name · fullname: ramda-(BETS)2GaCl4
shape · shape: 3
structure · str: BETS
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: 4.8
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: 3
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: 0.82
coherence length at 0 K for poly crystal · cohere: 87
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: OHC261
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 measured by micrwave loss. cohere for a*-c plane.
figure1 data file name · f1_filename: OHC261.dat
f2 data file name · f2_filename: —
title · title: Superconductivity and pseudogap states studied by microwave conductivity measurements of ramda-(BEDT-TSF)2GaCl4
year · year: 2006
keyword · keyword: —
institute · institute: Physics Department, Graduate School of Science, Tohoku University, Sendai 980-0845, Japan
journal · journal: Physica C, 440(2006)17
author · author: T.Suzuki,E.Negishi,H.Uozaki,H.Matsui,N.Toyota
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 262 · BETS

Tc: 5

Critical pressure, pcrit: 0 GPa

2001 · JP01308325

Method —

Inspect row 262: properties, remarks and source

Superconducting properties and Fermi-surface topology of the quasi-two-dimensional organic superconductor ramda-(BETS)2GaCl4 (BETS = bis(ethylene-dithio)tetraselenafulvalene)

J.Phys.:Condens.Matter, 13(2001)8325

Source remark: Hc2 measured for H//b*. dHvA effect, magnetoresistance, effective mass were measured. penet measured by LC inductance.

Common name (raw): GaCl4
Sample form: Single crystal bulk (code 3)
Coherence length at 0 K (raw): 14
Penetration depth at 0 K (raw): 150
GL parameter (source glpar) (raw): 107

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All 49 original cells and provenance

Original physical lines 247–247; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 12a80562fd40ddaa29bd7af5b85d0b199d408733255410dbe9158e3955f90468

data number · num: 262
reference number · refno: JP01308325
common formula of materials · name: GaCl4
full material name · fullname: ramda-(BETS)2GaCl4
shape · shape: 3
structure · str: BETS
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: 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: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 14
penetration depth at 0 K for poly crystal · penet: 150
Ginzburg-Landau order parameter · glpar: 107
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: OHC262
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 measured for H//b*. dHvA effect, magnetoresistance, effective mass were measured. penet measured by LC inductance.
figure1 data file name · f1_filename: OHC262.dat
f2 data file name · f2_filename: —
title · title: Superconducting properties and Fermi-surface topology of the quasi-two-dimensional organic superconductor ramda-(BETS)2GaCl4 (BETS = bis(ethylene-dithio)tetraselenafulvalene)
year · year: 2001
keyword · keyword: —
institute · institute: National High Magnetic Field Laboratory, Los Alamos National Laboratory, MS-E536, Los Alamos, NM 87545, USA
journal · journal: J.Phys.:Condens.Matter, 13(2001)8325
author · author: C.Mielke,J.Singleton,Moon-Sun Nam,N.Harrison,C.C.Agosta,B.Fravel,L.K.Montgomery
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 263 · BETS

Tc: 5

Critical pressure, pcrit: 0 GPa

2001 · SYN1200771

Method —

Inspect row 263: properties, remarks and source

In-plane anisotropy of the upper critical field of ramda-(BETS)2GaCl4

Synth.Metals, 120(2001)771

Source remark: Hc2 by resistive transition. cohere(out-of-plane) = 9 A from dHc2/dT.

Common name (raw): GaCl4
Sample form: Single crystal bulk (code 3)
Coherence length at 0 K (raw): 143

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All 49 original cells and provenance

Original physical lines 248–248; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: d629c5414654448d58b62637e3502df6edbd66677abea4f4a1204b8aac1f573f

data number · num: 263
reference number · refno: SYN1200771
common formula of materials · name: GaCl4
full material name · fullname: ramda-(BETS)2GaCl4
shape · shape: 3
structure · str: BETS
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: 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: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 143
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: OHC263
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 by resistive transition. cohere(out-of-plane) = 9 A from dHc2/dT.
figure1 data file name · f1_filename: OHC263.dat
f2 data file name · f2_filename: —
title · title: In-plane anisotropy of the upper critical field of ramda-(BETS)2GaCl4
year · year: 2001
keyword · keyword: —
institute · institute: Department of Physics,Kyoto University,Kyoto,Japan
journal · journal: Synth.Metals, 120(2001)771
author · author: T.Kawasaki,M.A.Tanatar,T.Ishiguro,H.Tanaka,A.Kobayashi,H.Kobayashi
sample · sample: —
comments · comments: —

beta''-(BEDO-TTF)3Cu2(NCS)3Row 264 · BEDO-TTF

Tc: 1.06

Critical pressure, pcrit: 0 GPa

1990 · INO0291599

Method —

Inspect row 264: properties, remarks and source

The first ambient pressure organic superconductor containing oxygen in the donor molecule, beta<m>-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K

Inorg.Chem., 29(1990)1599

Source remark: monoclinic sublattice. single crystals were prepared by electrocrystallization.

Common name (raw): Cu2(NCS)3
Sample form: Not supplied
Lattice a (raw): 4.237
Lattice b (raw): 33.481
Lattice c (raw): 5.273
Lattice β (raw): 97.94

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All 49 original cells and provenance

Original physical lines 249–249; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 0cd5ee60e83a75d33e11723285380a21a72cafbe64c4eb8cf3d7e06db12555e5

data number · num: 264
reference number · refno: INO0291599
common formula of materials · name: Cu2(NCS)3
full material name · fullname: beta''-(BEDO-TTF)3Cu2(NCS)3
shape · shape: —
structure · str: BEDO-TTF
lattice constant a · lata: 4.237
lattice constant b · latb: 33.481
lattice constant c · latc: 5.273
lattice alpha · alpha: —
lattice beta · beta: 97.94
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 1.06
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: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: monoclinic sublattice. single crystals were prepared by electrocrystallization.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: The first ambient pressure organic superconductor containing oxygen in the donor molecule, beta<m>-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K
year · year: 1990
keyword · keyword: —
institute · institute: —
journal · journal: Inorg.Chem., 29(1990)1599
author · author: M.A.Beno,H.H.Wang,A.M.Kini,K.D.Carlson,U.Geiser,W.K.Kwok,J.E.Thompson,J.M.Williams,J.Ren,M.H.Whangbo
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 265 · BEDT-TTF

Tc: 12.5
Maximum Tc: 12.5

Critical pressure, pcrit: 0.03 GPa
At maximum Tc, pmax (raw): 0.03

1990 · INO0293272

Method —

Inspect row 265: properties, remarks and source

From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, kappa-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K)

Inorg.Chem., 29(1990)3274

Source remark: space-G = Pnma. semicon-semicon transition at 42K. not SC down to 0.6K under ambient P.

Common name (raw): Cu[N(CN)2]Cl
Sample form: Not supplied
Lattice a (raw): 12.977
Lattice b (raw): 29.979
Lattice c (raw): 8.48
dTc/dP at P = 0 (raw): -34

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All 49 original cells and provenance

Original physical lines 250–250; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 8240e3811e8d8f44160e158698b6e5246190888d34b5ac123dd282958138824b

data number · num: 265
reference number · refno: INO0293272
common formula of materials · name: Cu[N(CN)2]Cl
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Cl
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: 12.977
lattice constant b · latb: 29.979
lattice constant c · latc: 8.48
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 12.5
maximum tc under pressure · tcmax: 12.5
applied pressure for tcmax · pmax: 0.03
Critical pressure/GPa at which Tc can be observed · pcrit: 0.03
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: -34
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: space-G = Pnma. semicon-semicon transition at 42K. not SC down to 0.6K under ambient P.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, kappa-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K)
year · year: 1990
keyword · keyword: —
institute · institute: —
journal · journal: Inorg.Chem., 29(1990)3274
author · author: J.M.Williams,A.M.Kini,H.H.Wang,K.D.Carlson,U.Geiser,L.K.Montgomery,G.J.Pyrka,D.M.Watkins,J.M.Kommers,S.J.Boryschuk,A.V.Strieby Crouch,W.K.Kwok,J.E..Schirber,D.L.Overmyer,D.Jung,M.H.Whangbo
sample · sample: —
comments · comments: —

(BEDO-TTF)2ReO4:(H2O)Row 266 · BEDO-TTF

Tc: 0.9

Critical pressure, pcrit: 0 GPa

1991 · SSC0800191

Method —

Inspect row 266: properties, remarks and source

(BEDO-TTF)2REO4(H2O): A NEW ORGANIC SUPERCONDUCTOR+

SOLID STATE COMMUN.,80(1991)191

Source remark: monoclinic phase. Tc by susceptibility. Resistive Tc(on) = 2.5 K. Three phase transitions at 213K, 90K, 35K.

Common name (raw): ReO4:(H2O)
Sample form: Not supplied
Lattice a (raw): 12.16
Lattice b (raw): 34.05
Lattice c (raw): 8.091
Lattice β (raw): 123.44

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All 49 original cells and provenance

Original physical lines 251–251; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 8e3a4b3fb289fc693c743c756efa38daa35f06ede7131d0545f375ea2df55dcf

data number · num: 266
reference number · refno: SSC0800191
common formula of materials · name: ReO4:(H2O)
full material name · fullname: (BEDO-TTF)2ReO4:(H2O)
shape · shape: —
structure · str: BEDO-TTF
lattice constant a · lata: 12.16
lattice constant b · latb: 34.05
lattice constant c · latc: 8.091
lattice alpha · alpha: —
lattice beta · beta: 123.44
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0.9
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: —
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: monoclinic phase. Tc by susceptibility. Resistive Tc(on) = 2.5 K. Three phase transitions at 213K, 90K, 35K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: (BEDO-TTF)2REO4(H2O): A NEW ORGANIC SUPERCONDUCTOR+
year · year: 1991
keyword · keyword: —
institute · institute: 3.PHYSIKALISCHES INSTITUT DER UNIVERSITAT STUTTGART,PFAFFENWALDRING 57,7000 STUTTGART 80,GERMANY
journal · journal: SOLID STATE COMMUN.,80(1991)191
author · author: B.NEBER,D.SCHWEITZER,H.J.KELLER,H.W.HELBERG,I.HEINEN,K.WINZER,S.KAHLICH,SONG EN LAN
sample · sample: —
comments · comments: —

beta'-Me4Sb[Pd(dmit)2]2Row 267 · Pd(dmit)2

Tc: 8.4
Maximum Tc: 8.4

Critical pressure, pcrit: 0.4 GPa
At maximum Tc, pmax (raw): 0.45

2005 · JPS0740412

Method —

Inspect row 267: properties, remarks and source

Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)

J.Phys.Soc.Jpn, 74(2005)412

Source remark: Me=CH3. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for hydrostatic-P (upto 15 kbar) and c*-axis pressure.

Common name (raw): Me4Sb
Sample form: Not supplied

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All 49 original cells and provenance

Original physical lines 252–252; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 06be3913760424965f529a61c277bf41bde52df1d2b59c757d8d39338dbd2a1e

data number · num: 267
reference number · refno: JPS0740412
common formula of materials · name: Me4Sb
full material name · fullname: beta'-Me4Sb[Pd(dmit)2]2
shape · shape: —
structure · str: Pd(dmit)2
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: 8.4
maximum tc under pressure · tcmax: 8.4
applied pressure for tcmax · pmax: 0.45
Critical pressure/GPa at which Tc can be observed · pcrit: 0.4
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: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Me=CH3. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for hydrostatic-P (upto 15 kbar) and c*-axis pressure.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)
year · year: 2005
keyword · keyword: —
institute · institute: Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan
journal · journal: J.Phys.Soc.Jpn, 74(2005)412
author · author: A.Tajima,A.Nakao,R.Kato
sample · sample: —
comments · comments: —

beta'-Me2Et2P[Pd(dmit)2]2Row 268 · Pd(dmit)2

Tc: 6.1
Maximum Tc: 6.1

Critical pressure, pcrit: 0.4 GPa
At maximum Tc, pmax (raw): 0.45

2005 · JPS0740412

Method —

Inspect row 268: properties, remarks and source

Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)

J.Phys.Soc.Jpn, 74(2005)412

Source remark: Me=CH3. Et=C2H5. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for a-axis pressure.

Common name (raw): Me2Et2P
Sample form: Not supplied

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All 49 original cells and provenance

Original physical lines 253–253; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 4defc10e585aa66aa7a9fcda86e3d63a78ab8641c7e4910e367a1fd62001af77

data number · num: 268
reference number · refno: JPS0740412
common formula of materials · name: Me2Et2P
full material name · fullname: beta'-Me2Et2P[Pd(dmit)2]2
shape · shape: —
structure · str: Pd(dmit)2
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: 6.1
maximum tc under pressure · tcmax: 6.1
applied pressure for tcmax · pmax: 0.45
Critical pressure/GPa at which Tc can be observed · pcrit: 0.4
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: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Me=CH3. Et=C2H5. SC-region: 4 < uniaxial-P(P//b-axis) < 10 kbar. not SC for a-axis pressure.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Uniaxial Strain Effects in the Conducting Pd(dmit)2 System: (dmit = 1,3-Dithiol-2-thione-4,5-dithiolate)
year · year: 2005
keyword · keyword: —
institute · institute: Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan
journal · journal: J.Phys.Soc.Jpn, 74(2005)412
author · author: A.Tajima,A.Nakao,R.Kato
sample · sample: —
comments · comments: —

beta'-Me4As[Pd(dmit)2]2Row 269 · Pd(dmit)2

Tc: 4

Critical pressure, pcrit: 0.7 GPa

2002 · P066020508

Method —

Inspect row 269: properties, remarks and source

Uniaxial strain effect in a strongly correlated two-dimensional system beta'-(CH3)4As[Pd(dmit)2]2

Phys.Rev.B, 66(2002)020508R

Source remark: Me=CH3. SC for b-axis pressure (7 < P < 10 kbar). not SC for a- and c-axis pressure.

Common name (raw): Me4As
Sample form: Not supplied

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All 49 original cells and provenance

Original physical lines 254–254; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: bb8d4035c1cd9a25f87968ecdbb072c80c49a1b3662b4f0f6deb26343b028135

data number · num: 269
reference number · refno: P066020508
common formula of materials · name: Me4As
full material name · fullname: beta'-Me4As[Pd(dmit)2]2
shape · shape: —
structure · str: Pd(dmit)2
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
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0.7
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: Me=CH3. SC for b-axis pressure (7 < P < 10 kbar). not SC for a- and c-axis pressure.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Uniaxial strain effect in a strongly correlated two-dimensional system beta'-(CH3)4As[Pd(dmit)2]2
year · year: 2002
keyword · keyword: —
institute · institute: Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama 351-0198,Japan
journal · journal: Phys.Rev.B, 66(2002)020508R
author · author: R.Kato,N.Tajima,M.Tamura,J.Yamaura
sample · sample: —
comments · comments: —

beta'-Me2Et2P[Pd(dmit)2]2Row 270 · Pd(dmit)2

Tc: 4

Critical pressure, pcrit: 0.69 GPa

1998 · SSC1050561

Method —

Inspect row 270: properties, remarks and source

A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)

Solid State Commun., 105(1998)561

Source remark: Me=CH3. Et=C2H5. SC-region: 6.9 =< P =< 10.4 kbar. Tc=1.8 K at P=10.4 kbar. R(H,T) measured at P=6.9 kbar. two dimensionality (r/B) = 0.82.

Common name (raw): Me2Et2P
Sample form: Not supplied
dTc/dP at P = 0 (raw): -6

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All 49 original cells and provenance

Original physical lines 255–255; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 9ab074f0144b1d79dac24ee87ba3a3d6a2a7822bfbf5b10c5ade7c1de806fc2d

data number · num: 270
reference number · refno: SSC1050561
common formula of materials · name: Me2Et2P
full material name · fullname: beta'-Me2Et2P[Pd(dmit)2]2
shape · shape: —
structure · str: Pd(dmit)2
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
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0.69
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: -6
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: Me=CH3. Et=C2H5. SC-region: 6.9 =< P =< 10.4 kbar. Tc=1.8 K at P=10.4 kbar. R(H,T) measured at P=6.9 kbar. two dimensionality (r/B) = 0.82.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)
year · year: 1998
keyword · keyword: —
institute · institute: ISSP, The University of Tokyo,Tokyo,Japan
journal · journal: Solid State Commun., 105(1998)561
author · author: R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima
sample · sample: —
comments · comments: —

beta'-Me2Et2Sb[Pd(dmit)2]2Row 271 · Pd(dmit)2

—

1998 · SSC1050561

Method —

Inspect row 271: properties, remarks and source

A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)

Solid State Commun., 105(1998)561

Source remark: Me=CH3. Et=C2H5. not SC upto 10.4 kbar. two dimensionality (r/B) = 0.96.

Common name (raw): Me2Et2Sb
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 256–256; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: c25477a08b59d5d70712beec02fdd93711a9c34ca288874fcd5111efde193a4b

data number · num: 271
reference number · refno: SSC1050561
common formula of materials · name: Me2Et2Sb
full material name · fullname: beta'-Me2Et2Sb[Pd(dmit)2]2
shape · shape: —
structure · str: Pd(dmit)2
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: —
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Me=CH3. Et=C2H5. not SC upto 10.4 kbar. two dimensionality (r/B) = 0.96.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: A new molecular superconductor beta'-Et2Me2P[Pd(dmit)2]2 (dmit=2-thioxo-1,3-dithiole-4,5-dithiolate)
year · year: 1998
keyword · keyword: —
institute · institute: ISSP, The University of Tokyo,Tokyo,Japan
journal · journal: Solid State Commun., 105(1998)561
author · author: R.Kato,Y.Kashimura,S.Aonuma,N.Hanasaki,H.Tajima
sample · sample: —
comments · comments: —

beta-(EDT-TTF)4Hg2.9I8Row 272 · EDT-TTF

Tc: 8.1

Critical pressure, pcrit: 0 GPa

2004 · SYN1400151

Method —

Inspect row 272: properties, remarks and source

New ambient pressure organic superconductor with Tc = 8.1 K based on unsymmetrical donor molecule, ethylenedithiotetrathiafulvalene: (EDT-TTF)4Hg3-zI8, z=0.1-0.2

Synth.Metals, 140(2004)151

Source remark: COHERE(0) estimated from COHERE(1.43K)//=126A. nCOHERE(0)=22A from nCOHERE(1.43K)=25A. stoichiometry determined by EPMA.

Common name (raw): Hg2.9I8
Sample form: Not supplied
Coherence length at 0 K (raw): 114

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All 49 original cells and provenance

Original physical lines 257–257; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: fd6bdd8a4c6798225d117f0c826efc716711f58877eb1d8bb484baf7adcb355a

data number · num: 272
reference number · refno: SYN1400151
common formula of materials · name: Hg2.9I8
full material name · fullname: beta-(EDT-TTF)4Hg2.9I8
shape · shape: —
structure · str: EDT-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: 8.1
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: 114
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: OHC272
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: COHERE(0) estimated from COHERE(1.43K)//=126A. nCOHERE(0)=22A from nCOHERE(1.43K)=25A. stoichiometry determined by EPMA.
figure1 data file name · f1_filename: OHC272.dat
f2 data file name · f2_filename: —
title · title: New ambient pressure organic superconductor with Tc = 8.1 K based on unsymmetrical donor molecule, ethylenedithiotetrathiafulvalene: (EDT-TTF)4Hg3-zI8, z=0.1-0.2
year · year: 2004
keyword · keyword: —
institute · institute: Institute of Problems of Chemical Physics, Russian Academy of Science, Chernogolovka 142432, MD, Russia
journal · journal: Synth.Metals, 140(2004)151
author · author: E.I.Zhilyaeva,S.A.Torunova,R.N.Lyubovskaya,G.A.Mousdis,G.C.Papavassiliou,J.A.A.J.Perenboom,S.I.Pesotskii,R.B.Lyubovskii
sample · sample: —
comments · comments: —

kappa-(BETS)2FeCl4Row 273 · BETS

Tc: 0.1

Critical pressure, pcrit: 0 GPa

2001 · CEM1590407

Method —

Inspect row 273: properties, remarks and source

Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions

J.Solid State Chem., 159(2001)407

Source remark: AF comfirmed by SP-heat. AF easy axis = a-axis.

Common name (raw): FeCl4
Sample form: Not supplied
Néel temperature (raw): 0.45

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All 49 original cells and provenance

Original physical lines 258–258; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: c4b0cf85de8a6a2611be618171a51261fb820246c8efa97eb1d444eb802679d3

data number · num: 273
reference number · refno: CEM1590407
common formula of materials · name: FeCl4
full material name · fullname: kappa-(BETS)2FeCl4
shape · shape: —
structure · str: BETS
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: 0.1
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: 0.45
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: AF comfirmed by SP-heat. AF easy axis = a-axis.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions
year · year: 2001
keyword · keyword: —
institute · institute: Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
journal · journal: J.Solid State Chem., 159(2001)407
author · author: T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi
sample · sample: —
comments · comments: —

kappa-(BETS)2FeBr4Row 274 · BETS

Tc: 1

Critical pressure, pcrit: 0 GPa

2001 · CEM1590407

Method —

Inspect row 274: properties, remarks and source

Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions

J.Solid State Chem., 159(2001)407

Source remark: oriented crystal

Common name (raw): 4-Feb
Sample form: Not supplied
Néel temperature (raw): 2.5

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All 49 original cells and provenance

Original physical lines 259–259; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6f215a1cb31f4b2c890a8931980e99665303041c4b4a9f516c548f36aed50943

data number · num: 274
reference number · refno: CEM1590407
common formula of materials · name: 4-Feb
full material name · fullname: kappa-(BETS)2FeBr4
shape · shape: —
structure · str: BETS
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
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: 2.5
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: oriented crystal
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Organic antiferromagnetic metals exhibiting superconducting transitions kappa-(BETS)2FeX4 (X=Cl,Br): Drastic effect of halogen substitution on the successive phase transitions
year · year: 2001
keyword · keyword: —
institute · institute: Research Centre for Spectrochemistry, School of Science, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
journal · journal: J.Solid State Chem., 159(2001)407
author · author: T.Otsuka,A.Kobayashi,Y.Miyamoto,J.Kiuchi,S.Nakamura,N.Wada,E.Fujiwara,H.Fujiwara,H.Kobayashi
sample · sample: —
comments · comments: —

(DMET)2Au(CN)2Row 275 · DMET

Tc: 0.8

Critical pressure, pcrit: 0.5 GPa

1987 · CHL0870931

Method —

Inspect row 275: properties, remarks and source

New organic superconductor, (DMET)2Au(CN)2

Chem.Lett., (1987)931

Source remark: M-I transition at 25K.

Common name (raw): Au(CN)2
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 260–260; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: febb124458d8cbacb873f8c7891daef9b4da689a12aa32133f94de8fe1f044db

data number · num: 275
reference number · refno: CHL0870931
common formula of materials · name: Au(CN)2
full material name · fullname: (DMET)2Au(CN)2
shape · shape: —
structure · str: DMET
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: 0.8
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0.5
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: M-I transition at 25K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New organic superconductor, (DMET)2Au(CN)2
year · year: 1987
keyword · keyword: —
institute · institute: —
journal · journal: Chem.Lett., (1987)931
author · author: K.Kikuchi,M.Kikuchi,T.Namiki,K.Saito,I.Ikemoto,K.Murata,T.Ishiguro,K.Kobayashi
sample · sample: —
comments · comments: —

kappa-(BETS)2GaBr4Row 276 · BETS

Tc: 1

Critical pressure, pcrit: 0 GPa

2000 · JMC0100245

Method —

Inspect row 276: properties, remarks and source

A new kappa-type organic superconductor based on BETS molecules, kappa- (BETS)2GaBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene]

J.Mater.Chem., 10(2000)245

Source remark: Tc=0.5 - 1.0 K. Tc(on) = 1.3 K. Space-G = Pnma

Common name (raw): GaBr4
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 261–261; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: d571a56b7076fc5371d6377d1c487dc756e6f2b856e0d5954f92b3112e97570e

data number · num: 276
reference number · refno: JMC0100245
common formula of materials · name: GaBr4
full material name · fullname: kappa-(BETS)2GaBr4
shape · shape: —
structure · str: BETS
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
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: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Tc=0.5 - 1.0 K. Tc(on) = 1.3 K. Space-G = Pnma
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: A new kappa-type organic superconductor based on BETS molecules, kappa- (BETS)2GaBr4 [BETS = bis(ethylenedithio)tetraselenafulvalene]
year · year: 2000
keyword · keyword: —
institute · institute: Institute for Molecular Science, Myodaiji-cho, Okazaki 444-8585, Japan
journal · journal: J.Mater.Chem., 10(2000)245
author · author: H.Tanaka,E.Ojima,H.Fujiwara,Y.Nakazawa,H.Kobayashi,A.Kobayashi
sample · sample: —
comments · comments: —

beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhNO2Row 277 · BEDT-TTF

Tc: 6.2

Critical pressure, pcrit: 0 GPa

2001 · JMC0112095

Method —

Inspect row 277: properties, remarks and source

New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)

J.Mater.Chem., 11(2001)2095

Source remark: space-G = C2/c. Curie-C = 3.877 emu/mole. Structure parameters are at 120 K.

Common name (raw): [(H3O)Fe(C2O4)3]:PhNO2
Sample form: Not supplied
Lattice a (raw): 10.2732
Lattice b (raw): 19.9494
Lattice c (raw): 35.0304
Lattice β (raw): 92.969
Curie temperature (raw): -0.16

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

All 49 original cells and provenance

Original physical lines 262–262; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 42a7f4e4ce52638c6b8313510940d36801176afeaa052cd3594faec15f0d33c6

data number · num: 277
reference number · refno: JMC0112095
common formula of materials · name: [(H3O)Fe(C2O4)3]:PhNO2
full material name · fullname: beta''-(BEDT-TTF)4[(H3O)Fe(C2O4)3]:PhNO2
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: 10.2732
lattice constant b · latb: 19.9494
lattice constant c · latc: 35.0304
lattice alpha · alpha: —
lattice beta · beta: 92.969
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 6.2
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: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: -0.16
Neel temperature · neelt: —
figure1 file name · fig1: —
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: space-G = C2/c. Curie-C = 3.877 emu/mole. Structure parameters are at 120 K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New superconducting charge-transfer salts (BEDTTTF)4[A:M(C2O4)3]:C6H5NO2 (A = H3O or NH4, M = Cr or Fe, BEDT-TTF = bis(ethylenedithio)tetrathiafulvalene)
year · year: 2001
keyword · keyword: —
institute · institute: Davy-Faraday Research Laboratory, The Royal Institution of Great Britain, 21 Albemarle Street, London, UK
journal · journal: J.Mater.Chem., 11(2001)2095
author · author: S.Rashid,S.S.Turner,P.Day,J.A.K.Howard,P.Guionneau,E.J.L.McInnes,F.E.Mabbs,R.J.H.Clark,S.Firth,T.Biggs
sample · sample: —
comments · comments: —