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 · 541–560 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
(BETS)2MnBr4Row 668 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 668: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: M-I transition at about 70 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnBr4, solvent=TCE. Common name (raw) MnBr4 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 543–543; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `2dd2a56691a3b42a378b513b714213da5d4a5db2531679d251a62b672b126744` data number · `num` 668 reference number · `refno` ACS1180368 common formula of materials · `name` MnBr4 full material name · `fullname` (BETS)2MnBr4 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` — 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` M-I transition at about 70 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnBr4, solvent=TCE. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) year · `year` 1996 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Okazaki 444, Japan journal · `journal` J.Am.Chem.Soc., 118(1996)368 author · `author` Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux sample · `sample` — comments · `comments` —
(BETS)2NiCl4Row 669 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 669: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: M-I transition at about 50 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)NiCl4, solvent=TCE. Common name (raw) NiCl4 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 544–544; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `767e601e0755c77be2713881d94ceab3e545fbb5167f5d38a0814fa8bc237adb` data number · `num` 669 reference number · `refno` ACS1180368 common formula of materials · `name` NiCl4 full material name · `fullname` (BETS)2NiCl4 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` — 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` M-I transition at about 50 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)NiCl4, solvent=TCE. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) year · `year` 1996 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Okazaki 444, Japan journal · `journal` J.Am.Chem.Soc., 118(1996)368 author · `author` Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux sample · `sample` — comments · `comments` —
(BETS)2CuCl4Row 670 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 670: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: Metallic for T > 4 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuCl4, solvent=TCE. Common name (raw) CuCl4 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 545–545; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `5e97fe64a929dcac43d34c66bf147893d05d4a16d79d595d92acf0c292d4c75c` data number · `num` 670 reference number · `refno` ACS1180368 common formula of materials · `name` CuCl4 full material name · `fullname` (BETS)2CuCl4 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` — 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` Metallic for T > 4 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuCl4, solvent=TCE. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) year · `year` 1996 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Okazaki 444, Japan journal · `journal` J.Am.Chem.Soc., 118(1996)368 author · `author` Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux sample · `sample` — comments · `comments` —
(BETS)2CuBr4Row 671 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 671: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: M-I transition at about 55 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuBr4, solvent=TCE. Common name (raw) CuBr4 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 546–546; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `eb0eb18b4d99e419a5f9d6afc20ad0ef6ce320a1c9a621e9efcf3ab55e6a1a38` data number · `num` 671 reference number · `refno` ACS1180368 common formula of materials · `name` CuBr4 full material name · `fullname` (BETS)2CuBr4 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` — 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` M-I transition at about 55 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuBr4, solvent=TCE. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) year · `year` 1996 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Okazaki 444, Japan journal · `journal` J.Am.Chem.Soc., 118(1996)368 author · `author` Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 675 · BEDT-TTF	Tc 9.5	Critical pressure, pcrit 0 GPa	2018 · PRB097024505 Method —
Inspect row 675: properties, remarks and source Quantum vortex melting and phase diagram in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 Phys.Rev.B, 97(2018)024505 Source remark: three phases: I(H<0.6T, R//=0 and R/n=0), II(0.6<H<4 T, R//=0 and R/n>0), III(4T,H,Hc2, R//>0 and R/n>0) Common name (raw) Cu(NCS)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 547–547; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `25bbe2f5cc2b5fc54715921d728e153a44ba44d0fc385d95974825a0c177bdd3` data number · `num` 675 reference number · `refno` PRB097024505 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 9.5 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` — 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` OHC675 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` three phases: I(H<0.6T, R//=0 and R/n=0), II(0.6<H<4 T, R//=0 and R/n>0), III(4T,H,Hc2, R//>0 and R/n>0) figure1 data file name · `f1_filename` OHC675.dat f2 data file name · `f2_filename` — title · `title` Quantum vortex melting and phase diagram in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2 year · `year` 2018 keyword · `keyword` — institute · `institute` National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan journal · `journal` Phys.Rev.B, 97(2018)024505 author · `author` S. Uji,Y. Fujii,S. Sugiura,T. Terashima,T. Isono,J. Yamada sample · `sample` — comments · `comments` —
beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2Row 676 · BEDT-TTF	Tc 4.8	Critical pressure, pcrit 0 GPa	2018 · PRB097144505 Method —
Inspect row 676: properties, remarks and source Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]C6H5NO2 Phys.Rev.B, 97(2018)144505 Source remark: Ph = C6H5. Hc2/n/ = 2.5 T. Hc2//=8.4Hc2/n/. FFLO state sudied by measuring resistivity and torque. H<FFLO> = 15 T = 3.1Tc. Common name (raw) [(H3O)Ga(C2O4)3]:PhNO2 Sample form Not supplied Lattice a (raw) 10.2782 Lattice b (raw) 19.8733 Lattice c (raw) 35.043 Lattice β (raw) 93.423 Hc2 at 0 K (raw) 21 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 548–548; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `3f15e23035a2f499a8b0974df2e342019a37af4c6e25803526512c800a13c9d6` data number · `num` 676 reference number · `refno` PRB097144505 common formula of materials · `name` [(H3O)Ga(C2O4)3]:PhNO2 full material name · `fullname` beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2 shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` 10.2782 lattice constant b · `latb` 19.8733 lattice constant c · `latc` 35.043 lattice alpha · `alpha` — lattice beta · `beta` 93.423 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` 21 -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` OHC676 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Ph = C6H5. Hc2/n/ = 2.5 T. Hc2//=8.4*Hc2/n/. FFLO state sudied by measuring resistivity and torque. H<FFLO> = 15 T = 3.1Tc. figure1 data file name · `f1_filename` OHC676.dat f2 data file name · `f2_filename` — title · `title` Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]C6H5NO2 year · `year` 2018 keyword · `keyword` — institute · `institute` National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan journal · `journal` Phys.Rev.B, 97(2018)144505 author · `author` S. Uji,Y. Iida,S. Sugiura,T. Isono,K. Sugii,N. Kikugawa,T. Terashima,S. Yasuzuka,H. Akutsu,Y. Nakazawa,D. Graf,P. Day sample · `sample` — comments · `comments` —
beta''-(BEDT-TTF)2SF5CH2CF2SO3Row 677 · BEDT-TTF	Tc 5.2	Critical pressure, pcrit 0 GPa	2016 · PRL116067003 Method —
Inspect row 677: properties, remarks and source Microscopic Study of the Fulde-Ferrell-Larkin-Ovchinnikov State in an All-Organic Superconductor Phys.Rev.Lett., 116(2016)067003 Source remark: From ref.16 in PRB097(2018)144505. Hc2/n/ = 1.3 T. Hc2//=11.5Hc2/n/. H<FFLO> = 9.5 T = 1.9Tc. Common name (raw) SF5CH2CF2SO3 Sample form Not supplied Hc2 at 0 K (raw) 14 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 549–549; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `e2ac2af81b5370c5dbc871561826fc23b7efd73db9959ace3103adcb153c2daf` data number · `num` 677 reference number · `refno` PRL116067003 common formula of materials · `name` SF5CH2CF2SO3 full material name · `fullname` beta''-(BEDT-TTF)2SF5CH2CF2SO3 shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 5.2 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=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` 14 -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` From ref.16 in PRB097(2018)144505. Hc2/n/ = 1.3 T. Hc2//=11.5*Hc2/n/. H<FFLO> = 9.5 T = 1.9Tc. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Microscopic Study of the Fulde-Ferrell-Larkin-Ovchinnikov State in an All-Organic Superconductor year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Physics and Astronomy, UCLA, Los Angeles, California 90095, USA journal · `journal` Phys.Rev.Lett., 116(2016)067003 author · `author` G. Koutroulakis,H. Kuhne,J.?A. Schlueter,J. Wosnitza,S.?E. Brown sample · `sample` — comments · `comments` —
EtMe3P[Pd(dmit)2]2Row 678 · [Pd(dmit)2	Tc 4.36	Critical pressure, pcrit 0 GPa	2018 · PRB097224502 Method —
Inspect row 678: properties, remarks and source Dimensionality of superconductivity in the layered organic material EtMe3P[Pd(dmit)2]2 under pressure Phys.Rev.B, 97(2018)224502 Source remark: Et=C2H5, Me=CH3. Hc2(T) for H//plane. For H/n, (dHc2/dT) = (1/6)2.7 (=value of dHc2/dT for H//plane). anisotropy factor m</n>/m<//> = 32. sample prepared by aerial oxidation method Common name (raw) EtMe3P Sample form Not supplied −dHc2/dT at Tc (raw) 2.7 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 550–550; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `f80b240e06cbe97c3ca274668c0e90e449d91f05a8e8f40526b5ad2e0b9729d2` data number · `num` 678 reference number · `refno` PRB097224502 common formula of materials · `name` EtMe3P full material name · `fullname` EtMe3P[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` 4.36 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` 2.7 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` OHC678 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Et=C2H5, Me=CH3. Hc2(T) for H//plane. For H/n, (dHc2/dT) = (1/6)*2.7 (=value of dHc2/dT for H//plane). anisotropy factor m</n>/m<//> = 32. sample prepared by aerial oxidation method figure1 data file name · `f1_filename` OHC678.dat f2 data file name · `f2_filename` — title · `title` Dimensionality of superconductivity in the layered organic material EtMe3P[Pd(dmit)2]2 under pressure year · `year` 2018 keyword · `keyword` — institute · `institute` Department of Applied Physics, Tokyo University of Science, Tokyo 125-8585, Japan journal · `journal` Phys.Rev.B, 97(2018)224502 author · `author` R. Yamamoto,Y. Yanagita,T. Namaizawa,S. Komuro,T. Furukawa,T. Itou,R. Kato sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 679 · BETS	Tc 4.8	Critical pressure, pcrit 0 GPa	2016 · JPS085043705 Method —
Inspect row 679: properties, remarks and source Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4 J.Phys.Soc.Jpn, 85(2016)043705 Source remark: gap 2d =4.30 kTc from SP. (dC/gammaTc) = 1.56. These data added to #652 Common name (raw) GaCl4 Sample form Not supplied Energy gap at 0 K (raw) 4.3 Electronic specific heat coefficient (raw) 20.6 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 551–551; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `d598bb312033c438521fba1938a6e30f9947dca7e6e158b416f16e4a734ad7ed` data number · `num` 679 reference number · `refno` JPS085043705 common formula of materials · `name` GaCl4 full material name · `fullname` ramda-(BETS)2GaCl4 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` 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` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` 4.3 method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` 20.6 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` gap 2d =4.30 kTc from SP. (dC/gamma*Tc) = 1.56. These data added to #652 figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4 year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan journal · `journal` J.Phys.Soc.Jpn, 85(2016)043705 author · `author` Shusaku Imajo,Naoki Kanda,Satoshi Yamashita,Hiroki Akutsu,Yasuhiro Nakazawa,Hiroya Kumagai,Takuya Kobayashi,Atsushi Kawamoto sample · `sample` — comments · `comments` —
(TMTSF)2(ClO4)1-x(ReO4)x: x=0.07Row 680 · TMTSF	Tc 0.83	Critical pressure, pcrit 0 GPa	2018 · PRB098115111 Method —
Inspect row 680: properties, remarks and source Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 Phys.Rev.B, 98(2018)115111 Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content) Common name (raw) ClO4-ReO4 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 552–552; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `d4ebb41c4d9b335dcfe443db7daae88f906fd7df4dfe14d6d8a002f5934530b7` data number · `num` 680 reference number · `refno` PRB098115111 common formula of materials · `name` ClO4-ReO4 full material name · `fullname` (TMTSF)2(ClO4)1-x(ReO4)x: x=0.07 shape · `shape` — structure · `str` TMTSF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0.83 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=AM^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — 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 decreases and resistivity (along c axis) increase with increasing x (ReO4-content) figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 year · `year` 2018 keyword · `keyword` — institute · `institute` Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria journal · `journal` Phys.Rev.B, 98(2018)115111 author · `author` Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome sample · `sample` — comments · `comments` —
(TMTSF)2(ClO4)1-x(ReO4)x: x=0.06Row 681 · TMTSF	Tc 0.77	Critical pressure, pcrit 0 GPa	2018 · PRB098115111 Method —
Inspect row 681: properties, remarks and source Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 Phys.Rev.B, 98(2018)115111 Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content) Common name (raw) ClO4-ReO4 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 553–553; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `67e6221b03c0e6bfd31b9d166450e80d084fc29d77a780b203a10d9ed4d710be` data number · `num` 681 reference number · `refno` PRB098115111 common formula of materials · `name` ClO4-ReO4 full material name · `fullname` (TMTSF)2(ClO4)1-x(ReO4)x: x=0.06 shape · `shape` — structure · `str` TMTSF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0.77 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=AM^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — 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 decreases and resistivity (along c axis) increase with increasing x (ReO4-content) figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 year · `year` 2018 keyword · `keyword` — institute · `institute` Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria journal · `journal` Phys.Rev.B, 98(2018)115111 author · `author` Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome sample · `sample` — comments · `comments` —
(TMTSF)2(ClO4)1-x(ReO4)x: x=0.1Row 682 · TMTSF	Tc 0.39	Critical pressure, pcrit 0 GPa	2018 · PRB098115111 Method —
Inspect row 682: properties, remarks and source Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 Phys.Rev.B, 98(2018)115111 Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content) Common name (raw) ClO4-ReO4 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 554–554; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `52f3898001a174c15e20ee126acb85e5d1f3270f2c453e595191a823194a7553` data number · `num` 682 reference number · `refno` PRB098115111 common formula of materials · `name` ClO4-ReO4 full material name · `fullname` (TMTSF)2(ClO4)1-x(ReO4)x: x=0.1 shape · `shape` — structure · `str` TMTSF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 0.39 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=AM^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — 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 decreases and resistivity (along c axis) increase with increasing x (ReO4-content) figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 year · `year` 2018 keyword · `keyword` — institute · `institute` Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria journal · `journal` Phys.Rev.B, 98(2018)115111 author · `author` Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome sample · `sample` — comments · `comments` —
(TMTSF)2(ClO4)1-x(ReO4)x: x = 0Row 683 · TMTSF	Tc 1.58	Critical pressure, pcrit 0 GPa	2018 · PRB098115111 Method —
Inspect row 683: properties, remarks and source Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 Phys.Rev.B, 98(2018)115111 Source remark: Kyoto-sample. Tc(zero) = 1.19 K Common name (raw) ClO4-ReO4 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 555–555; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `155bf7ce2c6115db6926c51884447e340e370063121b3a494a441b0d80630aab` data number · `num` 683 reference number · `refno` PRB098115111 common formula of materials · `name` ClO4-ReO4 full material name · `fullname` (TMTSF)2(ClO4)1-x(ReO4)x: x = 0 shape · `shape` — structure · `str` TMTSF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 1.58 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` Kyoto-sample. Tc(zero) = 1.19 K figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 year · `year` 2018 keyword · `keyword` — institute · `institute` Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria journal · `journal` Phys.Rev.B, 98(2018)115111 author · `author` Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome sample · `sample` — comments · `comments` —
(TMTSF)2(ClO4)1-x(ReO4)x: x = 0Row 684 · TMTSF	Tc 1.35	Critical pressure, pcrit 0 GPa	2018 · PRB098115111 Method —
Inspect row 684: properties, remarks and source Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 Phys.Rev.B, 98(2018)115111 Source remark: Orsay-sample . Tc(zero) = 1.08 K. resistivity (along c* axis) larger than Kyoto-sample Common name (raw) ClO4-ReO4 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 556–556; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `0a1eb21ab2d0f9f2dac070a32f343326a53936cfb63f864348d4c6b4314a7cba` data number · `num` 684 reference number · `refno` PRB098115111 common formula of materials · `name` ClO4-ReO4 full material name · `fullname` (TMTSF)2(ClO4)1-x(ReO4)x: x = 0 shape · `shape` — structure · `str` TMTSF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 1.35 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=AM^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — 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` Orsay-sample . Tc(zero) = 1.08 K. resistivity (along c axis) larger than Kyoto-sample figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4 year · `year` 2018 keyword · `keyword` — institute · `institute` Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria journal · `journal` Phys.Rev.B, 98(2018)115111 author · `author` Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu(NCS)2Row 685 · BEDT-TTF	Tc 10.2	Critical pressure, pcrit 0 GPa	2000 · PRB0610750 Method —
Inspect row 685: properties, remarks and source Paramagnetic limiting of the upper critical field of the layered organic superconductor kappa -(BEDT-TTF)2Cu(SCN)2 Phys.Rev.B, 61(2000)750 Source remark: Hc2 defined as R = 1 Ohm(Hc2) and R-cross point (H). Boss diffinitions give the same (dHc2/dT) value. Pauli limit discussed in details Common name (raw) Cu(NCS)2 Sample form Not supplied Hc2 at 0 K (raw) 30 −dHc2/dT at Tc (raw) 3 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 557–557; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `eb862aa1ac0aa9999afdf9b98ea22c8c3aeba4c6f136494d1ac7be484ed72059` data number · `num` 685 reference number · `refno` PRB0610750 common formula of materials · `name` Cu(NCS)2 full material name · `fullname` kappa-(BEDT-TTF)2Cu(NCS)2 shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 10.2 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=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` 30 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` 3 coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OHC685A figure2 filename · `fig2` OHC685B figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2 defined as R = 1 Ohm(Hc2) and R-cross point (H*). Boss diffinitions give the same (dHc2/dT) value. Pauli limit discussed in details figure1 data file name · `f1_filename` OHC685A.dat f2 data file name · `f2_filename` OHC685B.dat title · `title` Paramagnetic limiting of the upper critical field of the layered organic superconductor kappa -(BEDT-TTF)2Cu(SCN)2 year · `year` 2000 keyword · `keyword` — institute · `institute` Department of Physics, University of Miami, Coral Gables, Florida 33124 journal · `journal` Phys.Rev.B, 61(2000)750 author · `author` F. Zuo,J. S. Brooks,Ross H. McKenzie,J. A. Schlueter,Jack M. Williams sample · `sample` — comments · `comments` —
ramda-(BETS)2FeCl4Row 686 · BETS	Tc 2.1	—	2012 · PRB085174530 Method —
Inspect row 686: properties, remarks and source Magnetic torque studies on FFLO phase in magnetic-field-induced organic superconductor lambda-(BETS)2FeCl4 Phys.Rev.B, 85(2012)174530 Source remark: H-induced SC. Tc(in DB) shows tricritical point. FFLO state appears in SC region. Phase diagram shows for H//c. Common name (raw) FeCl4 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 558–558; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `9e041c4d679038326bcd8fdafcab9572420e13f98b0e52b4d7c6377eeb7ff955` data number · `num` 686 reference number · `refno` PRB085174530 common formula of materials · `name` FeCl4 full material name · `fullname` ramda-(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` 2.1 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` OPH686 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` H-induced SC. Tc(in DB) shows tricritical point. FFLO state appears in SC region. Phase diagram shows for H//c. figure1 data file name · `f1_filename` OPH686.dat f2 data file name · `f2_filename` — title · `title` Magnetic torque studies on FFLO phase in magnetic-field-induced organic superconductor lambda-(BETS)2FeCl4 year · `year` 2012 keyword · `keyword` — institute · `institute` National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan journal · `journal` Phys.Rev.B, 85(2012)174530 author · `author` S. Uji,K. Kodama,K. Sugii,T. Terashima,Y. Takahide,N. Kurita,S. Tsuchiya,M. Kimata,A. Kobayashi,B. Zhou,H. Kobayashi sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 687 · BEDT-TTF	Tc 12	Critical pressure, pcrit 0 GPa	2018 · JPS087123704 Method —
Inspect row 687: properties, remarks and source Superconducting Phase Diagram of the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br above 30T J.Phys.Soc.Jpn, 87(2018)123704 Source remark: Hc2,dHc2/dT for H/n/plane. cohere//, cohere/n/ = 3 A. out-of-plane resistance (I//b-axis) measured. C<el>/gammaTc = 3.3 Common name (raw) Cu[N(CN)2]Br Sample form Not supplied Hc2 at 0 K (raw) 7 −dHc2/dT at Tc (raw) 0.6 Coherence length at 0 K (raw) 70 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 559–559; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `aa8cf830eac8890ae7665013b38f8b02e55ed32ee91a5233cccbe9232e056581` data number · `num` 687 reference number · `refno` JPS087123704 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 12 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` 7 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` 0.6 coherence length at 0 K for poly crystal · `cohere` 70 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` OHC687-1 figure2 filename · `fig2` OHC687-2 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Hc2,dHc2/dT for H/n/plane. cohere//, cohere/n/ = 3 A. out-of-plane resistance (I//b-axis) measured. C<el>/gamma*Tc = 3.3 figure1 data file name · `f1_filename` OHC687-1.dat f2 data file name · `f2_filename` OHC687-2.dat title · `title` Superconducting Phase Diagram of the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br above 30T year · `year` 2018 keyword · `keyword` — institute · `institute` The Institute for Solid State Physics, the University of Tokyo, Kashiwa, Chiba 277-8581, Japan journal · `journal` J.Phys.Soc.Jpn, 87(2018)123704 author · `author` Shusaku Imajo,Yasuhiro Nakazawa,Koichi Kindo sample · `sample` — comments · `comments` —
(beta)''-(BEDT-TTF)2SF5CH2CF2SO3Row 700 · BEDT-TTF	Tc 5.2	—	2019 · PRB100014515 Method —
Inspect row 700: properties, remarks and source Josephson vortex dynamics and Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta-(BEDT-TTF)2SF5CH2CF2SO3 Phys.Rev.B., 100(2019)014515 Source remark: Tc = 4.7 - 5.2 K. Hc2//ab = 14 T, Hc2/n/ab = 1.3 T. H<FFLO> = 9.5 - 10 T. T<FFLO>/Tc = 1.9 - 2.1 T/K. Common name (raw) SF5CH2CF2SO3 Sample form Single crystal bulk (code 3) Hc2 at 0 K (raw) 14 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 560–560; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `be05fc9e8a259ea02e453ffaa7ed1a603898087bcbf37262ffd08e4239a05767` data number · `num` 700 reference number · `refno` PRB100014515 common formula of materials · `name` SF5CH2CF2SO3 full material name · `fullname` (beta)''-(BEDT-TTF)2SF5CH2CF2SO3 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` 5.2 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` 14 -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` OHC700 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Tc = 4.7 - 5.2 K. Hc2//ab = 14 T, Hc2/n/ab = 1.3 T. H<FFLO> = 9.5 - 10 T. T<FFLO>/Tc = 1.9 - 2.1 T/K. figure1 data file name · `f1_filename` OHC700.dat f2 data file name · `f2_filename` — title · `title` Josephson vortex dynamics and Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta-(BEDT-TTF)2SF5CH2CF2SO3 year · `year` 2019 keyword · `keyword` — institute · `institute` National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan journal · `journal` Phys.Rev.B., 100(2019)014515 author · `author` Shiori Sugiura,Taichi Terashima,Shinya Uji,Syuma Yasuzuka,John A. Schlueter sample · `sample` — comments · `comments` —
alpha-(BEDT-TTF)2NH4Hg(SCN)4Row 1001 · BEDT-TTF	Tc 0.95	—	1998 · PR05703623 Method —
Inspect row 1001: properties, remarks and source Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy Phys.Rev.B,57(1998)3623 Source remark: out-of-plane coherence = 1400 micron. Anysotropy factor=2000. Inter layer spacing=20 A. Common name (raw) NH4Hg(SCN)4 Sample form Single crystal bulk (code 3) −dHc2/dT at Tc (raw) 0.08 Coherence length at 0 K (raw) 500 Penetration depth at 0 K (raw) 0.7 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 561–561; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6aa297969ce3715d4967d05f8b72ff4b7bc31aa9eeebbe837e7296a0965a41f3` data number · `num` 1001 reference number · `refno` PR05703623 common formula of materials · `name` NH4Hg(SCN)4 full material name · `fullname` alpha-(BEDT-TTF)2NH4Hg(SCN)4 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` 0.95 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` 0.08 coherence length at 0 K for poly crystal · `cohere` 500 penetration depth at 0 K for poly crystal · `penet` 0.7 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` specific heat C/T vs T table file name · `tbl` — table description · `tblname` — comment · `commt` out-of-plane coherence = 1400 micron. Anysotropy factor=2000. Inter layer spacing=20 A. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy year · `year` 1998 keyword · `keyword` — institute · `institute` Institute for Molecular Science, Myodaiji, Okazaki 444, Japan journal · `journal` Phys.Rev.B,57(1998)3623 author · `author` H.Taniguchi,Hiromi Taniguchi,K.Kanoda,Kazushi Kanoda,Y.Nakazawa,Yasuhiro Nakazawa sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 1002 · BEDT-TTF	Tc 12.6 Maximum Tc 12.6	Critical pressure, pcrit 0.019 GPa	1996 · JPS0652987 Method —
Inspect row 1002: properties, remarks and source Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure J.Phys.Soc.Jpn, 65(1996)2987 Source remark: hydrogenated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=19 MPa. SC-1 to SC at P=30 MPa. Common name (raw) Cu[N(CN)2]Cl Sample form Single crystal bulk (code 3) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 562–562; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `10526c2cc27528c4d839c3a60a298318eaa6ac60b7bc7d6deac027d0f75a0f2a` data number · `num` 1002 reference number · `refno` JPS0652987 common formula of materials · `name` Cu[N(CN)2]Cl full material name · `fullname` kappa-(BEDT-TTF)2Cu[N(CN)2]Cl shape · `shape` 3 structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 12.6 maximum tc under pressure · `tcmax` 12.6 applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0.019 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` OPH1002 figure2 filename · `fig2` — figure description · `figname` phase diagram table file name · `tbl` — table description · `tblname` — comment · `commt` hydrogenated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=19 MPa. SC-1 to SC at P=30 MPa. figure1 data file name · `f1_filename` OPH1002.dat f2 data file name · `f2_filename` — title · `title` Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure year · `year` 1996 keyword · `keyword` — institute · `institute` Kyoto University, Kyoto,Japan journal · `journal` J.Phys.Soc.Jpn, 65(1996)2987 author · `author` H.Ito,T.Ishiguro,M.Kubota,G.Saito sample · `sample` — comments · `comments` —

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

(BETS)2MnBr4Row 668 · BETS

—

1996 · ACS1180368

Method —

Inspect row 668: properties, remarks and source

New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)

J.Am.Chem.Soc., 118(1996)368

Source remark: M-I transition at about 70 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnBr4, solvent=TCE.

Common name (raw): MnBr4
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 543–543; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 2dd2a56691a3b42a378b513b714213da5d4a5db2531679d251a62b672b126744

data number · num: 668
reference number · refno: ACS1180368
common formula of materials · name: MnBr4
full material name · fullname: (BETS)2MnBr4
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: —
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: M-I transition at about 70 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnBr4, solvent=TCE.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)
year · year: 1996
keyword · keyword: —
institute · institute: Institute for Molecular Science, Okazaki 444, Japan
journal · journal: J.Am.Chem.Soc., 118(1996)368
author · author: Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux
sample · sample: —
comments · comments: —

(BETS)2NiCl4Row 669 · BETS

—

1996 · ACS1180368

Method —

Inspect row 669: properties, remarks and source

New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)

J.Am.Chem.Soc., 118(1996)368

Source remark: M-I transition at about 50 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)NiCl4, solvent=TCE.

Common name (raw): NiCl4
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 544–544; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 767e601e0755c77be2713881d94ceab3e545fbb5167f5d38a0814fa8bc237adb

data number · num: 669
reference number · refno: ACS1180368
common formula of materials · name: NiCl4
full material name · fullname: (BETS)2NiCl4
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: —
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: M-I transition at about 50 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)NiCl4, solvent=TCE.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)
year · year: 1996
keyword · keyword: —
institute · institute: Institute for Molecular Science, Okazaki 444, Japan
journal · journal: J.Am.Chem.Soc., 118(1996)368
author · author: Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux
sample · sample: —
comments · comments: —

(BETS)2CuCl4Row 670 · BETS

—

1996 · ACS1180368

Method —

Inspect row 670: properties, remarks and source

New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)

J.Am.Chem.Soc., 118(1996)368

Source remark: Metallic for T > 4 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuCl4, solvent=TCE.

Common name (raw): CuCl4
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 545–545; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 5e97fe64a929dcac43d34c66bf147893d05d4a16d79d595d92acf0c292d4c75c

data number · num: 670
reference number · refno: ACS1180368
common formula of materials · name: CuCl4
full material name · fullname: (BETS)2CuCl4
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: —
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: Metallic for T > 4 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuCl4, solvent=TCE.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)
year · year: 1996
keyword · keyword: —
institute · institute: Institute for Molecular Science, Okazaki 444, Japan
journal · journal: J.Am.Chem.Soc., 118(1996)368
author · author: Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux
sample · sample: —
comments · comments: —

(BETS)2CuBr4Row 671 · BETS

—

1996 · ACS1180368

Method —

Inspect row 671: properties, remarks and source

New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)

J.Am.Chem.Soc., 118(1996)368

Source remark: M-I transition at about 55 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuBr4, solvent=TCE.

Common name (raw): CuBr4
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 546–546; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: eb0eb18b4d99e419a5f9d6afc20ad0ef6ce320a1c9a621e9efcf3ab55e6a1a38

data number · num: 671
reference number · refno: ACS1180368
common formula of materials · name: CuBr4
full material name · fullname: (BETS)2CuBr4
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: —
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: M-I transition at about 55 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CuBr4, solvent=TCE.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene)
year · year: 1996
keyword · keyword: —
institute · institute: Institute for Molecular Science, Okazaki 444, Japan
journal · journal: J.Am.Chem.Soc., 118(1996)368
author · author: Hayao Kobayashi,Hideto Tomita,Toshio Naito,Akiko Kobayashi,Fumiko Sakai,Tokuko Watanabe,Patrick Cassoux
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 675 · BEDT-TTF

Tc: 9.5

Critical pressure, pcrit: 0 GPa

2018 · PRB097024505

Method —

Inspect row 675: properties, remarks and source

Quantum vortex melting and phase diagram in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2

Phys.Rev.B, 97(2018)024505

Source remark: three phases: I(H<0.6T, R//=0 and R/n=0), II(0.6<H<4 T, R//=0 and R/n>0), III(4T,H,Hc2, R//>0 and R/n>0)

Common name (raw): Cu(NCS)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 547–547; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 25bbe2f5cc2b5fc54715921d728e153a44ba44d0fc385d95974825a0c177bdd3

data number · num: 675
reference number · refno: PRB097024505
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 9.5
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: —
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: OHC675
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: three phases: I(H<0.6T, R//=0 and R/n=0), II(0.6<H<4 T, R//=0 and R/n>0), III(4T,H,Hc2, R//>0 and R/n>0)
figure1 data file name · f1_filename: OHC675.dat
f2 data file name · f2_filename: —
title · title: Quantum vortex melting and phase diagram in the layered organic superconductor kappa-(BEDT-TTF)2Cu(NCS)2
year · year: 2018
keyword · keyword: —
institute · institute: National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan
journal · journal: Phys.Rev.B, 97(2018)024505
author · author: S. Uji,Y. Fujii,S. Sugiura,T. Terashima,T. Isono,J. Yamada
sample · sample: —
comments · comments: —

beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2Row 676 · BEDT-TTF

Tc: 4.8

Critical pressure, pcrit: 0 GPa

2018 · PRB097144505

Method —

Inspect row 676: properties, remarks and source

Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]C6H5NO2

Phys.Rev.B, 97(2018)144505

Source remark: Ph = C6H5. Hc2/n/ = 2.5 T. Hc2//=8.4*Hc2/n/. FFLO state sudied by measuring resistivity and torque. H<FFLO> = 15 T = 3.1Tc.

Common name (raw): [(H3O)Ga(C2O4)3]:PhNO2
Sample form: Not supplied
Lattice a (raw): 10.2782
Lattice b (raw): 19.8733
Lattice c (raw): 35.043
Lattice β (raw): 93.423
Hc2 at 0 K (raw): 21

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

All 49 original cells and provenance

Original physical lines 548–548; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 3f15e23035a2f499a8b0974df2e342019a37af4c6e25803526512c800a13c9d6

data number · num: 676
reference number · refno: PRB097144505
common formula of materials · name: [(H3O)Ga(C2O4)3]:PhNO2
full material name · fullname: beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: 10.2782
lattice constant b · latb: 19.8733
lattice constant c · latc: 35.043
lattice alpha · alpha: —
lattice beta · beta: 93.423
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: 21
-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: OHC676
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Ph = C6H5. Hc2/n/ = 2.5 T. Hc2//=8.4*Hc2/n/. FFLO state sudied by measuring resistivity and torque. H<FFLO> = 15 T = 3.1Tc.
figure1 data file name · f1_filename: OHC676.dat
f2 data file name · f2_filename: —
title · title: Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]C6H5NO2
year · year: 2018
keyword · keyword: —
institute · institute: National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan and Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan
journal · journal: Phys.Rev.B, 97(2018)144505
author · author: S. Uji,Y. Iida,S. Sugiura,T. Isono,K. Sugii,N. Kikugawa,T. Terashima,S. Yasuzuka,H. Akutsu,Y. Nakazawa,D. Graf,P. Day
sample · sample: —
comments · comments: —

beta''-(BEDT-TTF)2SF5CH2CF2SO3Row 677 · BEDT-TTF

Tc: 5.2

Critical pressure, pcrit: 0 GPa

2016 · PRL116067003

Method —

Inspect row 677: properties, remarks and source

Microscopic Study of the Fulde-Ferrell-Larkin-Ovchinnikov State in an All-Organic Superconductor

Phys.Rev.Lett., 116(2016)067003

Source remark: From ref.16 in PRB097(2018)144505. Hc2/n/ = 1.3 T. Hc2//=11.5*Hc2/n/. H<FFLO> = 9.5 T = 1.9Tc.

Common name (raw): SF5CH2CF2SO3
Sample form: Not supplied
Hc2 at 0 K (raw): 14

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

All 49 original cells and provenance

Original physical lines 549–549; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: e2ac2af81b5370c5dbc871561826fc23b7efd73db9959ace3103adcb153c2daf

data number · num: 677
reference number · refno: PRL116067003
common formula of materials · name: SF5CH2CF2SO3
full material name · fullname: beta''-(BEDT-TTF)2SF5CH2CF2SO3
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 5.2
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: 14
-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: From ref.16 in PRB097(2018)144505. Hc2/n/ = 1.3 T. Hc2//=11.5*Hc2/n/. H<FFLO> = 9.5 T = 1.9Tc.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Microscopic Study of the Fulde-Ferrell-Larkin-Ovchinnikov State in an All-Organic Superconductor
year · year: 2016
keyword · keyword: —
institute · institute: Department of Physics and Astronomy, UCLA, Los Angeles, California 90095, USA
journal · journal: Phys.Rev.Lett., 116(2016)067003
author · author: G. Koutroulakis,H. Kuhne,J.?A. Schlueter,J. Wosnitza,S.?E. Brown
sample · sample: —
comments · comments: —

EtMe3P[Pd(dmit)2]2Row 678 · [Pd(dmit)2

Tc: 4.36

Critical pressure, pcrit: 0 GPa

2018 · PRB097224502

Method —

Inspect row 678: properties, remarks and source

Dimensionality of superconductivity in the layered organic material EtMe3P[Pd(dmit)2]2 under pressure

Phys.Rev.B, 97(2018)224502

Source remark: Et=C2H5, Me=CH3. Hc2(T) for H//plane. For H/n, (dHc2/dT) = (1/6)*2.7 (=value of dHc2/dT for H//plane). anisotropy factor m</n>/m<//> = 32. sample prepared by aerial oxidation method

Common name (raw): EtMe3P
Sample form: Not supplied
−dHc2/dT at Tc (raw): 2.7

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

All 49 original cells and provenance

Original physical lines 550–550; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: f80b240e06cbe97c3ca274668c0e90e449d91f05a8e8f40526b5ad2e0b9729d2

data number · num: 678
reference number · refno: PRB097224502
common formula of materials · name: EtMe3P
full material name · fullname: EtMe3P[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: 4.36
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: 2.7
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: OHC678
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Et=C2H5, Me=CH3. Hc2(T) for H//plane. For H/n, (dHc2/dT) = (1/6)*2.7 (=value of dHc2/dT for H//plane). anisotropy factor m</n>/m<//> = 32. sample prepared by aerial oxidation method
figure1 data file name · f1_filename: OHC678.dat
f2 data file name · f2_filename: —
title · title: Dimensionality of superconductivity in the layered organic material EtMe3P[Pd(dmit)2]2 under pressure
year · year: 2018
keyword · keyword: —
institute · institute: Department of Applied Physics, Tokyo University of Science, Tokyo 125-8585, Japan
journal · journal: Phys.Rev.B, 97(2018)224502
author · author: R. Yamamoto,Y. Yanagita,T. Namaizawa,S. Komuro,T. Furukawa,T. Itou,R. Kato
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 679 · BETS

Tc: 4.8

Critical pressure, pcrit: 0 GPa

2016 · JPS085043705

Method —

Inspect row 679: properties, remarks and source

Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4

J.Phys.Soc.Jpn, 85(2016)043705

Source remark: gap 2d =4.30 kTc from SP. (dC/gamma*Tc) = 1.56. These data added to #652

Common name (raw): GaCl4
Sample form: Not supplied
Energy gap at 0 K (raw): 4.3
Electronic specific heat coefficient (raw): 20.6

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

All 49 original cells and provenance

Original physical lines 551–551; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: d598bb312033c438521fba1938a6e30f9947dca7e6e158b416f16e4a734ad7ed

data number · num: 679
reference number · refno: JPS085043705
common formula of materials · name: GaCl4
full material name · fullname: ramda-(BETS)2GaCl4
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: 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: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: 4.3
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: 20.6
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: gap 2d =4.30 kTc from SP. (dC/gamma*Tc) = 1.56. These data added to #652
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Thermodynamic Evidence of d-Wave Superconductivity of the Organic Superconductor ramda-(BETS)2GaCl4
year · year: 2016
keyword · keyword: —
institute · institute: Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan
journal · journal: J.Phys.Soc.Jpn, 85(2016)043705
author · author: Shusaku Imajo,Naoki Kanda,Satoshi Yamashita,Hiroki Akutsu,Yasuhiro Nakazawa,Hiroya Kumagai,Takuya Kobayashi,Atsushi Kawamoto
sample · sample: —
comments · comments: —

(TMTSF)2(ClO4)1-x(ReO4)x: x=0.07Row 680 · TMTSF

Tc: 0.83

Critical pressure, pcrit: 0 GPa

2018 · PRB098115111

Method —

Inspect row 680: properties, remarks and source

Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4

Phys.Rev.B, 98(2018)115111

Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)

Common name (raw): ClO4-ReO4
Sample form: Not supplied

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All 49 original cells and provenance

Original physical lines 552–552; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: d4ebb41c4d9b335dcfe443db7daae88f906fd7df4dfe14d6d8a002f5934530b7

data number · num: 680
reference number · refno: PRB098115111
common formula of materials · name: ClO4-ReO4
full material name · fullname: (TMTSF)2(ClO4)1-x(ReO4)x: x=0.07
shape · shape: —
structure · str: TMTSF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0.83
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 decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4
year · year: 2018
keyword · keyword: —
institute · institute: Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria
journal · journal: Phys.Rev.B, 98(2018)115111
author · author: Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome
sample · sample: —
comments · comments: —

(TMTSF)2(ClO4)1-x(ReO4)x: x=0.06Row 681 · TMTSF

Tc: 0.77

Critical pressure, pcrit: 0 GPa

2018 · PRB098115111

Method —

Inspect row 681: properties, remarks and source

Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4

Phys.Rev.B, 98(2018)115111

Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)

Common name (raw): ClO4-ReO4
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 553–553; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 67e6221b03c0e6bfd31b9d166450e80d084fc29d77a780b203a10d9ed4d710be

data number · num: 681
reference number · refno: PRB098115111
common formula of materials · name: ClO4-ReO4
full material name · fullname: (TMTSF)2(ClO4)1-x(ReO4)x: x=0.06
shape · shape: —
structure · str: TMTSF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0.77
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 decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4
year · year: 2018
keyword · keyword: —
institute · institute: Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria
journal · journal: Phys.Rev.B, 98(2018)115111
author · author: Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome
sample · sample: —
comments · comments: —

(TMTSF)2(ClO4)1-x(ReO4)x: x=0.1Row 682 · TMTSF

Tc: 0.39

Critical pressure, pcrit: 0 GPa

2018 · PRB098115111

Method —

Inspect row 682: properties, remarks and source

Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4

Phys.Rev.B, 98(2018)115111

Source remark: Tc decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)

Common name (raw): ClO4-ReO4
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 554–554; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 52f3898001a174c15e20ee126acb85e5d1f3270f2c453e595191a823194a7553

data number · num: 682
reference number · refno: PRB098115111
common formula of materials · name: ClO4-ReO4
full material name · fullname: (TMTSF)2(ClO4)1-x(ReO4)x: x=0.1
shape · shape: —
structure · str: TMTSF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 0.39
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 decreases and resistivity (along c* axis) increase with increasing x (ReO4-content)
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4
year · year: 2018
keyword · keyword: —
institute · institute: Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria
journal · journal: Phys.Rev.B, 98(2018)115111
author · author: Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome
sample · sample: —
comments · comments: —

(TMTSF)2(ClO4)1-x(ReO4)x: x = 0Row 683 · TMTSF

Tc: 1.58

Critical pressure, pcrit: 0 GPa

2018 · PRB098115111

Method —

Inspect row 683: properties, remarks and source

Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4

Phys.Rev.B, 98(2018)115111

Source remark: Kyoto-sample. Tc(zero) = 1.19 K

Common name (raw): ClO4-ReO4
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 555–555; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 155bf7ce2c6115db6926c51884447e340e370063121b3a494a441b0d80630aab

data number · num: 683
reference number · refno: PRB098115111
common formula of materials · name: ClO4-ReO4
full material name · fullname: (TMTSF)2(ClO4)1-x(ReO4)x: x = 0
shape · shape: —
structure · str: TMTSF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 1.58
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: Kyoto-sample. Tc(zero) = 1.19 K
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4
year · year: 2018
keyword · keyword: —
institute · institute: Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria
journal · journal: Phys.Rev.B, 98(2018)115111
author · author: Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome
sample · sample: —
comments · comments: —

(TMTSF)2(ClO4)1-x(ReO4)x: x = 0Row 684 · TMTSF

Tc: 1.35

Critical pressure, pcrit: 0 GPa

2018 · PRB098115111

Method —

Inspect row 684: properties, remarks and source

Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4

Phys.Rev.B, 98(2018)115111

Source remark: Orsay-sample . Tc(zero) = 1.08 K. resistivity (along c* axis) larger than Kyoto-sample

Common name (raw): ClO4-ReO4
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 556–556; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 0a1eb21ab2d0f9f2dac070a32f343326a53936cfb63f864348d4c6b4314a7cba

data number · num: 684
reference number · refno: PRB098115111
common formula of materials · name: ClO4-ReO4
full material name · fullname: (TMTSF)2(ClO4)1-x(ReO4)x: x = 0
shape · shape: —
structure · str: TMTSF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 1.35
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: Orsay-sample . Tc(zero) = 1.08 K. resistivity (along c* axis) larger than Kyoto-sample
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Influence of carrier lifetime on quantum criticality and superconducting Tc of (TMTSF)2ClO4
year · year: 2018
keyword · keyword: —
institute · institute: Universite Dr Tahar Moulay Saida, B.P. 138 cite ENNASR 20000, Saida, Algeria
journal · journal: Phys.Rev.B, 98(2018)115111
author · author: Abdelouahab Sedeki,Pascale Auban-Senzier,Shingo Yonezawa,Claude Bourbonnais,Denis Jerome
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu(NCS)2Row 685 · BEDT-TTF

Tc: 10.2

Critical pressure, pcrit: 0 GPa

2000 · PRB0610750

Method —

Inspect row 685: properties, remarks and source

Paramagnetic limiting of the upper critical field of the layered organic superconductor kappa -(BEDT-TTF)2Cu(SCN)2

Phys.Rev.B, 61(2000)750

Source remark: Hc2 defined as R = 1 Ohm(Hc2) and R-cross point (H*). Boss diffinitions give the same (dHc2/dT) value. Pauli limit discussed in details

Common name (raw): Cu(NCS)2
Sample form: Not supplied
Hc2 at 0 K (raw): 30
−dHc2/dT at Tc (raw): 3

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

All 49 original cells and provenance

Original physical lines 557–557; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: eb862aa1ac0aa9999afdf9b98ea22c8c3aeba4c6f136494d1ac7be484ed72059

data number · num: 685
reference number · refno: PRB0610750
common formula of materials · name: Cu(NCS)2
full material name · fullname: kappa-(BEDT-TTF)2Cu(NCS)2
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 10.2
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: 30
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: 3
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OHC685A
figure2 filename · fig2: OHC685B
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2 defined as R = 1 Ohm(Hc2) and R-cross point (H*). Boss diffinitions give the same (dHc2/dT) value. Pauli limit discussed in details
figure1 data file name · f1_filename: OHC685A.dat
f2 data file name · f2_filename: OHC685B.dat
title · title: Paramagnetic limiting of the upper critical field of the layered organic superconductor kappa -(BEDT-TTF)2Cu(SCN)2
year · year: 2000
keyword · keyword: —
institute · institute: Department of Physics, University of Miami, Coral Gables, Florida 33124
journal · journal: Phys.Rev.B, 61(2000)750
author · author: F. Zuo,J. S. Brooks,Ross H. McKenzie,J. A. Schlueter,Jack M. Williams
sample · sample: —
comments · comments: —

ramda-(BETS)2FeCl4Row 686 · BETS

Tc: 2.1

—

2012 · PRB085174530

Method —

Inspect row 686: properties, remarks and source

Magnetic torque studies on FFLO phase in magnetic-field-induced organic superconductor lambda-(BETS)2FeCl4

Phys.Rev.B, 85(2012)174530

Source remark: H-induced SC. Tc(in DB) shows tricritical point. FFLO state appears in SC region. Phase diagram shows for H//c.

Common name (raw): FeCl4
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 558–558; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 9e041c4d679038326bcd8fdafcab9572420e13f98b0e52b4d7c6377eeb7ff955

data number · num: 686
reference number · refno: PRB085174530
common formula of materials · name: FeCl4
full material name · fullname: ramda-(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: 2.1
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: OPH686
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: H-induced SC. Tc(in DB) shows tricritical point. FFLO state appears in SC region. Phase diagram shows for H//c.
figure1 data file name · f1_filename: OPH686.dat
f2 data file name · f2_filename: —
title · title: Magnetic torque studies on FFLO phase in magnetic-field-induced organic superconductor lambda-(BETS)2FeCl4
year · year: 2012
keyword · keyword: —
institute · institute: National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan
journal · journal: Phys.Rev.B, 85(2012)174530
author · author: S. Uji,K. Kodama,K. Sugii,T. Terashima,Y. Takahide,N. Kurita,S. Tsuchiya,M. Kimata,A. Kobayashi,B. Zhou,H. Kobayashi
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]BrRow 687 · BEDT-TTF

Tc: 12

Critical pressure, pcrit: 0 GPa

2018 · JPS087123704

Method —

Inspect row 687: properties, remarks and source

Superconducting Phase Diagram of the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br above 30T

J.Phys.Soc.Jpn, 87(2018)123704

Source remark: Hc2,dHc2/dT for H/n/plane. cohere//, cohere/n/ = 3 A. out-of-plane resistance (I//b-axis) measured. C<el>/gamma*Tc = 3.3

Common name (raw): Cu[N(CN)2]Br
Sample form: Not supplied
Hc2 at 0 K (raw): 7
−dHc2/dT at Tc (raw): 0.6
Coherence length at 0 K (raw): 70

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

All 49 original cells and provenance

Original physical lines 559–559; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: aa8cf830eac8890ae7665013b38f8b02e55ed32ee91a5233cccbe9232e056581

data number · num: 687
reference number · refno: JPS087123704
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 12
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: 7
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: 0.6
coherence length at 0 K for poly crystal · cohere: 70
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: OHC687-1
figure2 filename · fig2: OHC687-2
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Hc2,dHc2/dT for H/n/plane. cohere//, cohere/n/ = 3 A. out-of-plane resistance (I//b-axis) measured. C<el>/gamma*Tc = 3.3
figure1 data file name · f1_filename: OHC687-1.dat
f2 data file name · f2_filename: OHC687-2.dat
title · title: Superconducting Phase Diagram of the Organic Superconductor kappa-(BEDT-TTF)2Cu[N(CN)2]Br above 30T
year · year: 2018
keyword · keyword: —
institute · institute: The Institute for Solid State Physics, the University of Tokyo, Kashiwa, Chiba 277-8581, Japan
journal · journal: J.Phys.Soc.Jpn, 87(2018)123704
author · author: Shusaku Imajo,Yasuhiro Nakazawa,Koichi Kindo
sample · sample: —
comments · comments: —

(beta)''-(BEDT-TTF)2SF5CH2CF2SO3Row 700 · BEDT-TTF

Tc: 5.2

—

2019 · PRB100014515

Method —

Inspect row 700: properties, remarks and source

Josephson vortex dynamics and Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta-(BEDT-TTF)2SF5CH2CF2SO3

Phys.Rev.B., 100(2019)014515

Source remark: Tc = 4.7 - 5.2 K. Hc2//ab = 14 T, Hc2/n/ab = 1.3 T. H<FFLO> = 9.5 - 10 T. T<FFLO>/Tc = 1.9 - 2.1 T/K.

Common name (raw): SF5CH2CF2SO3
Sample form: Single crystal bulk (code 3)
Hc2 at 0 K (raw): 14

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

All 49 original cells and provenance

Original physical lines 560–560; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: be05fc9e8a259ea02e453ffaa7ed1a603898087bcbf37262ffd08e4239a05767

data number · num: 700
reference number · refno: PRB100014515
common formula of materials · name: SF5CH2CF2SO3
full material name · fullname: (beta)''-(BEDT-TTF)2SF5CH2CF2SO3
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: 5.2
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: 14
-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: OHC700
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Tc = 4.7 - 5.2 K. Hc2//ab = 14 T, Hc2/n/ab = 1.3 T. H<FFLO> = 9.5 - 10 T. T<FFLO>/Tc = 1.9 - 2.1 T/K.
figure1 data file name · f1_filename: OHC700.dat
f2 data file name · f2_filename: —
title · title: Josephson vortex dynamics and Fulde-Ferrell-Larkin-Ovchinnikov superconductivity in the layered organic superconductor beta-(BEDT-TTF)2SF5CH2CF2SO3
year · year: 2019
keyword · keyword: —
institute · institute: National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan
journal · journal: Phys.Rev.B., 100(2019)014515
author · author: Shiori Sugiura,Taichi Terashima,Shinya Uji,Syuma Yasuzuka,John A. Schlueter
sample · sample: —
comments · comments: —

alpha-(BEDT-TTF)2NH4Hg(SCN)4Row 1001 · BEDT-TTF

Tc: 0.95

—

1998 · PR05703623

Method —

Inspect row 1001: properties, remarks and source

Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy

Phys.Rev.B,57(1998)3623

Source remark: out-of-plane coherence = 1400 micron. Anysotropy factor=2000. Inter layer spacing=20 A.

Common name (raw): NH4Hg(SCN)4
Sample form: Single crystal bulk (code 3)
−dHc2/dT at Tc (raw): 0.08
Coherence length at 0 K (raw): 500
Penetration depth at 0 K (raw): 0.7

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

All 49 original cells and provenance

Original physical lines 561–561; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6aa297969ce3715d4967d05f8b72ff4b7bc31aa9eeebbe837e7296a0965a41f3

data number · num: 1001
reference number · refno: PR05703623
common formula of materials · name: NH4Hg(SCN)4
full material name · fullname: alpha-(BEDT-TTF)2NH4Hg(SCN)4
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: 0.95
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: 0.08
coherence length at 0 K for poly crystal · cohere: 500
penetration depth at 0 K for poly crystal · penet: 0.7
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: specific heat C/T vs T
table file name · tbl: —
table description · tblname: —
comment · commt: out-of-plane coherence = 1400 micron. Anysotropy factor=2000. Inter layer spacing=20 A.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Phase diagram of vortices in the quasi-two-dimensional organic superconductor alpha-(BEDT-TTF)2NH4Hg(SCN)4: Asystem of pancake vortices with out-of-plane coupling dominated by the electromagnetic energy
year · year: 1998
keyword · keyword: —
institute · institute: Institute for Molecular Science, Myodaiji, Okazaki 444, Japan
journal · journal: Phys.Rev.B,57(1998)3623
author · author: H.Taniguchi,Hiromi Taniguchi,K.Kanoda,Kazushi Kanoda,Y.Nakazawa,Yasuhiro Nakazawa
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2Cu[N(CN)2]ClRow 1002 · BEDT-TTF

Tc: 12.6
Maximum Tc: 12.6

Critical pressure, pcrit: 0.019 GPa

1996 · JPS0652987

Method —

Inspect row 1002: properties, remarks and source

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

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

Source remark: hydrogenated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=19 MPa. SC-1 to SC at P=30 MPa.

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

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

All 49 original cells and provenance

Original physical lines 562–562; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 10526c2cc27528c4d839c3a60a298318eaa6ac60b7bc7d6deac027d0f75a0f2a

data number · num: 1002
reference number · refno: JPS0652987
common formula of materials · name: Cu[N(CN)2]Cl
full material name · fullname: kappa-(BEDT-TTF)2Cu[N(CN)2]Cl
shape · shape: 3
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 12.6
maximum tc under pressure · tcmax: 12.6
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0.019
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: OPH1002
figure2 filename · fig2: —
figure description · figname: phase diagram
table file name · tbl: —
table description · tblname: —
comment · commt: hydrogenated sample. Tc is nealy independent on P. Incomplete superconductivity SC-II to SC-I at P=19 MPa. SC-1 to SC at P=30 MPa.
figure1 data file name · f1_filename: OPH1002.dat
f2 data file name · f2_filename: —
title · title: Metal-Nonmetal Transition and Superconductivity Localization in the Two-Dimensional Conductor kappa-(BEDT-TTF)2Cu[N(CN)2]Cl under Pressure
year · year: 1996
keyword · keyword: —
institute · institute: Kyoto University, Kyoto,Japan
journal · journal: J.Phys.Soc.Jpn, 65(1996)2987
author · author: H.Ito,T.Ishiguro,M.Kubota,G.Saito
sample · sample: —
comments · comments: —