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 · 521–540 shown

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

Organic source rows with separate transition and pressure columns; raw units are not inferred
Source material	Transition values (raw)	Pressure context	Reference / method
kappa-(d-[3:3]BEDT-TTF)2Cu[N(CN)2]BrRow 642 · BEDT-TTF	Tc 11.9	—	2015 · JPS084064713 Method —
Inspect row 642: properties, remarks and source Tunneling Spectroscopy in Organic Superconductor kappa-(BEDT-TTF-d[3,3])2Cu[N(CN)2]Br J.Phys.Soc.Jpn, 84(2015)064713 Source remark: Energy gap measured by STS(tunneling spectroscopy) at 1.2 K on the a-c plane. gap d(0) = 4.0 meV Common name (raw) Cu[N(CN)2]Br Sample form Not supplied Energy gap at 0 K (raw) 7.8 Gap method Tunneling (code 1) Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 523–523; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `7f1145416597d125b3e4ceaf4ef95bbc66ce05ea6b826cdfcdd50a0c91770379` data number · `num` 642 reference number · `refno` JPS084064713 common formula of materials · `name` Cu[N(CN)2]Br full material name · `fullname` kappa-(d-[3:3]BEDT-TTF)2Cu[N(CN)2]Br shape · `shape` — structure · `str` BEDT-TTF lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 11.9 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` 7.8 method of measuring energy gap · `gapmeth` 1 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` Energy gap measured by STS(tunneling spectroscopy) at 1.2 K on the a-c plane. gap d(0) = 4.0 meV figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Tunneling Spectroscopy in Organic Superconductor kappa-(BEDT-TTF-d[3,3])2Cu[N(CN)2]Br year · `year` 2015 keyword · `keyword` — institute · `institute` Department of Physics, Hokkaido University, Sapporo 060-0810, Japan journal · `journal` J.Phys.Soc.Jpn, 84(2015)064713 author · `author` Yuki Oka,Hiroyoshi Nobukane,Noriaki Matsunaga,Kazushige Nomura,Kazuhiro Katono,Koichi Ichimura,Atsushi Kawamoto sample · `sample` — comments · `comments` —
beta''-(BEDT)2SF5CH2CF2SO3Row 643 · BEDT-TTF	Tc 5.1	Critical pressure, pcrit 0 GPa	2015 · JPS084094709 Method —
Inspect row 643: properties, remarks and source In-Plane Anisotropy of Upper Critical Field and Flux-Flow Resistivity in Layered Organic Superconductor beta''-(ET)2SF5CH2CF2SO3 J.Phys.Soc.Jpn, 84(2015)094709 Source remark: Anisotropy and angular dependence of Hc2 were measured. Sample A (Tc=5.1K), B (Tc= 5.2 K) Common name (raw) SF5CH2CF2SO3 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 524–524; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `3dda349ed6f94d1a16e6a0698e0fd5e67525e663c38749cdeb54f55878efe165` data number · `num` 643 reference number · `refno` JPS084094709 common formula of materials · `name` SF5CH2CF2SO3 full material name · `fullname` beta''-(BEDT)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` 5.1 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` 0 tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OHC643-1 figure2 filename · `fig2` OHC643-2 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Anisotropy and angular dependence of Hc2 were measured. Sample A (Tc=5.1K), B (Tc= 5.2 K) figure1 data file name · `f1_filename` OHC643-1.dat f2 data file name · `f2_filename` OHC643-2.dat title · `title` In-Plane Anisotropy of Upper Critical Field and Flux-Flow Resistivity in Layered Organic Superconductor beta''-(ET)2SF5CH2CF2SO3 year · `year` 2015 keyword · `keyword` — institute · `institute` Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan journal · `journal` J.Phys.Soc.Jpn, 84(2015)094709 author · `author` Syuma Yasuzuka,Shinya Uji,Taichi Terashima,Kaori Sugii,Takayuki Isono,Yoritsugu Iida,John A. Schlueter sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 644 · BETS	Tc 6	—	2015 · JPS084104709 Method —
Inspect row 644: properties, remarks and source Vortex Dynamics and Diamagnetic Torque Signals in Two Dimensional Organic Superconductor ramda-(BETS)2GaCl4 J.Phys.Soc.Jpn, 84(2015)104709 Source remark: RRR = 300. R(T) max at 80 K. R-peak appears below Tc(onset) and depends on angle between ac-plane and b. H//c (defined as R(onset) ) measured . Common name (raw) GaCl4 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 525–525; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `f1ddc4f6bca87114b1d3458db5610491c67c5d6a2ac7aaa177b2d080ba3216d9` data number · `num` 644 reference number · `refno` JPS084104709 common formula of materials · `name` GaCl4 full material name · `fullname` ramda-(BETS)2GaCl4 shape · `shape` 3 structure · `str` BETS lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 6 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=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` OHC644 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` RRR = 300. R(T) max at 80 K. R-peak appears below Tc(onset) and depends on angle between ac-plane and b*. H//c (defined as R(onset) ) measured . figure1 data file name · `f1_filename` OHC644.dat f2 data file name · `f2_filename` — title · `title` Vortex Dynamics and Diamagnetic Torque Signals in Two Dimensional Organic Superconductor ramda-(BETS)2GaCl4 year · `year` 2015 keyword · `keyword` — institute · `institute` National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan journal · `journal` J.Phys.Soc.Jpn, 84(2015)104709 author · `author` Shinya Uji,Kouta Kodama,Kaori Sugii1,Taichi Terashima,Takahide Yamaguchi,Nobuyuki Kurita,Satoshi Tsuchiya,Takako Konoike,Motoi Kimata,Akiko Kobayashi,Biao Zhou,Hayao Kobayashi sample · `sample` — comments · `comments` —
K3-piceneRow 645 · picene	Tc 14	Critical pressure, pcrit 0 GPa	2015 · PHC5140199 Method —
Inspect row 645: properties, remarks and source Superconductivity in aromatic hydrocarbons Physica C, 514(2015)199 Source remark: SC-volume = 3.9% at 2K. Common name (raw) K3 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 526–526; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `dbc914cb31a06fe4dff4887dc36d7a19c9f810022fff686b653d40e17b8dabab` data number · `num` 645 reference number · `refno` PHC5140199 common formula of materials · `name` K3 full material name · `fullname` K3-picene shape · `shape` — structure · `str` picene lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 14 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` SC-volume = 3.9% at 2K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in aromatic hydrocarbons year · `year` 2015 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Physica C, 514(2015)199 author · `author` Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu sample · `sample` — comments · `comments` —
K3-[7]phenaceneRow 646 · phenacene	Tc 11	Critical pressure, pcrit 0 GPa	2015 · PHC5140199 Method —
Inspect row 646: properties, remarks and source Superconductivity in aromatic hydrocarbons Physica C, 514(2015)199 Source remark: SC-volume = 0.1% at 2K. Common name (raw) K3 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 527–527; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `d1c10c15aea7f6749b87e0e52a90835f34ed9291c76efc39523ea73a1a5081fa` data number · `num` 646 reference number · `refno` PHC5140199 common formula of materials · `name` K3 full material name · `fullname` K3-[7]phenacene shape · `shape` — structure · `str` phenacene lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 11 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` SC-volume = 0.1% at 2K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in aromatic hydrocarbons year · `year` 2015 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Physica C, 514(2015)199 author · `author` Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu sample · `sample` — comments · `comments` —
Sr1.5-phenanthreneRow 647 · phenanthrene	Tc 6	Critical pressure, pcrit 0 GPa	2015 · PHC5140199 Method —
Inspect row 647: properties, remarks and source Superconductivity in aromatic hydrocarbons Physica C, 514(2015)199 Source remark: SC-volume = 4% at 2K. Tc(SUS) = 5.3 K. Common name (raw) Sr1.5 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 528–528; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `c51c37b3a354604513349bed67c03091ee690418323963cb66b24babbc1c681e` data number · `num` 647 reference number · `refno` PHC5140199 common formula of materials · `name` Sr1.5 full material name · `fullname` Sr1.5-phenanthrene shape · `shape` — structure · `str` phenanthrene lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 6 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` SC-volume = 4% at 2K. Tc(SUS) = 5.3 K. figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in aromatic hydrocarbons year · `year` 2015 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Physica C, 514(2015)199 author · `author` Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu sample · `sample` — comments · `comments` —
Kx-DBPRow 648 · DBP	Tc 30	Critical pressure, pcrit 0 GPa	2015 · PHC5140199 Method —
Inspect row 648: properties, remarks and source Superconductivity in aromatic hydrocarbons Physica C, 514(2015)199 Source remark: Sample has two-phases: Tc1 = 30K, Tc2 = 7K. , corresponding to different x in Kx-DBP. DBP = dibenzopentacene Common name (raw) Kx 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 529–529; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `614970b136dbe269aba19311b984fceed66879b5c282026a9d7ca91efc888f8e` data number · `num` 648 reference number · `refno` PHC5140199 common formula of materials · `name` Kx full material name · `fullname` Kx-DBP shape · `shape` — structure · `str` DBP 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` 30 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` Sample has two-phases: Tc1 = 30K, Tc2 = 7K. , corresponding to different x in Kx-DBP. DBP = dibenzopentacene figure1 data file name · `f1_filename` — f2 data file name · `f2_filename` — title · `title` Superconductivity in aromatic hydrocarbons year · `year` 2015 keyword · `keyword` — institute · `institute` Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan journal · `journal` Physica C, 514(2015)199 author · `author` Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu sample · `sample` — comments · `comments` —
beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2Row 650 · BEDT-TTF	Tc 7.5	Critical pressure, pcrit 0 GPa	2016 · JPS085014601 Method —
Inspect row 650: properties, remarks and source High-Temperature Charge and Structure Anomalies in (beta)''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]/C6H5NO2 J.Phys.Soc.Jpn, 85(2016)014601 Source remark: There exist the kink at 90 K in C(T) and lattice parameters due to charge ordering. Debye-T = 130 K for T < 50 K fittong. Common name (raw) [(H3O)Ga(C2O4)3]:PhNO2 Sample form Not supplied Lattice a (raw) 10.251 Lattice b (raw) 20.05 Lattice c (raw) 35.19 Lattice β (raw) 92.326 Debye temperature (raw) 130 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 530–530; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `7eee12f98c70e189f50b8e28952e322b08c4d972c584c84206141a619d538e06` data number · `num` 650 reference number · `refno` JPS085014601 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` 10.251 lattice constant b · `latb` 20.05 lattice constant c · `latc` 35.19 lattice alpha · `alpha` — lattice beta · `beta` 92.326 lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 7.5 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` 130 Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OSP650 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` There exist the kink at 90 K in C(T) and lattice parameters due to charge ordering. Debye-T = 130 K for T < 50 K fittong. figure1 data file name · `f1_filename` OSP650.dat f2 data file name · `f2_filename` — title · `title` High-Temperature Charge and Structure Anomalies in (beta)''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]/C6H5NO2 year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Condensed Matter Physics, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan journal · `journal` J.Phys.Soc.Jpn, 85(2016)014601 author · `author` Yoshihiko Ihara,Yosuke Futami,Atsushi Kawamoto sample · `sample` — comments · `comments` —
ramda-(BETS)2FeCl4Row 651 · BETS	—	Critical pressure, pcrit 0 GPa	2016 · JPS085023601 Method —
Inspect row 651: properties, remarks and source Effective Field Study of Canted Antiferromagnetic Insulating Phase in Magnetic Organic Conductor ramda-(BETS)2FeCl4 through Specific Heat Measurement J.Phys.Soc.Jpn, 85(2016)023601 Source remark: H-induced SC. (dC) = C - C(lattice) measured under H//c. Tn obtained from the peak of (dC) for 3 samples for H < 11T Common name (raw) FeCl4 Sample form Not supplied Néel temperature (raw) 8.4 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 531–531; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `f3a0c194638930330bdd951f46a74200c80ead9f2746c552d77ade6e207eb0ac` data number · `num` 651 reference number · `refno` JPS085023601 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` — 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` 8.4 figure1 file name · `fig1` OPH651 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` H-induced SC. (dC) = C - C(lattice) measured under H//c. Tn obtained from the peak of (dC) for 3 samples for H < 11T figure1 data file name · `f1_filename` OPH651.dat f2 data file name · `f2_filename` — title · `title` Effective Field Study of Canted Antiferromagnetic Insulating Phase in Magnetic Organic Conductor ramda-(BETS)2FeCl4 through Specific Heat Measurement year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Physics, Toho University, Funabashi, Chiba 274-8510, Japan journal · `journal` J.Phys.Soc.Jpn, 85(2016)023601 author · `author` Kazuo Shimada,Naoya Tajima,Koji Kajita,Yutaka Nishio sample · `sample` — comments · `comments` —
ramda-(BETS)2GaCl4Row 652 · BETS	Tc 4.8	Critical pressure, pcrit 0 GPa	2016 · JPS085043705 Method —
Inspect row 652: 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: C = aT + bT^3 + cT^5 + Einstein term(E1, E2): b = 18.2 mJ/mol.K4, c = 0.024 mJ/mol.K6, E1 = 30.6 K, E2 = 46.7 K from data fitting. Common name (raw) GaCl4 Sample form Not supplied Hc2 at 0 K (raw) 3.5 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 532–532; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `6c9acb78cfa620cd6e0dfe13b6934837c88dc249507eeca0ccab68538f8a35ce` data number · `num` 652 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` 3.5 -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` 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` C = aT + bT^3 + c*T^5 + Einstein term(E1, E2): b = 18.2 mJ/mol.K4, c = 0.024 mJ/mol.K6, E1 = 30.6 K, E2 = 46.7 K from data fitting. 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` —
kappa-(BEDT-TTF)2CF3SO3Row 655 · BEDT-TTF	Tc 4.7 Maximum Tc 4.8	Critical pressure, pcrit 1.1 GPa At maximum Tc, pmax (raw) 1.3	2016 · PRB094020503 Method —
Inspect row 655: properties, remarks and source Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice Phys.Rev.B, 94(2016)020503 Source remark: SC-data at P = 1.45 GPa. Hc2 defined as midpoint. Hc2 depend on current direction Common name (raw) CF3SO3 Sample form Single crystal bulk (code 3) Coherence length at 0 K (raw) 370 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 533–533; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `f9fe2d33f57d11a82dfe573f5b36cd1564444480d2a1901357daa67b9acdff1a` data number · `num` 655 reference number · `refno` PRB094020503 common formula of materials · `name` CF3SO3 full material name · `fullname` kappa-(BEDT-TTF)2CF3SO3 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` 4.7 maximum tc under pressure · `tcmax` 4.8 applied pressure for tcmax · `pmax` 1.3 Critical pressure/GPa at which Tc can be observed · `pcrit` 1.1 tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 370 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` OHC655 figure2 filename · `fig2` OTC655 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` SC-data at P = 1.45 GPa. Hc2 defined as midpoint. Hc2 depend on current direction figure1 data file name · `f1_filename` OHC655.dat f2 data file name · `f2_filename` OTC655.dat title · `title` Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan journal · `journal` Phys.Rev.B, 94(2016)020503 author · `author` Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito sample · `sample` — comments · `comments` —
kappa-(BEDT-TTF)2CF3SO3Row 656 · BEDT-TTF	Tc 4.98 Maximum Tc 4.98	Critical pressure, pcrit 1.6 GPa At maximum Tc, pmax (raw) 1.9	2016 · PRB094020503 Method —
Inspect row 656: properties, remarks and source Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice Phys.Rev.B, 94(2016)020503 Source remark: Tc for c-axis pressure (strain) Common name (raw) CF3SO3 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 534–534; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `93a09a2f5fa4bad10fc9581ac35099ed68e0af46d59be758294ccffa302ca501` data number · `num` 656 reference number · `refno` PRB094020503 common formula of materials · `name` CF3SO3 full material name · `fullname` kappa-(BEDT-TTF)2CF3SO3 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` 4.98 maximum tc under pressure · `tcmax` 4.98 applied pressure for tcmax · `pmax` 1.9 Critical pressure/GPa at which Tc can be observed · `pcrit` 1.6 tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` — figure1 file name · `fig1` OTC656 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Tc for c-axis pressure (strain) figure1 data file name · `f1_filename` OTC656.dat f2 data file name · `f2_filename` — title · `title` Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice year · `year` 2016 keyword · `keyword` — institute · `institute` Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan journal · `journal` Phys.Rev.B, 94(2016)020503 author · `author` Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito sample · `sample` — comments · `comments` —
lambda-(BETS)2Fe0.63Ga0.37Cl4Row 660 · BETS	Tc 5.05	—	2017 · PRB095165133 Method —
Inspect row 660: properties, remarks and source Internal field effect on vortex states in the layered organic superconductor lambda-(BETS)2Fe1-xGaxCl4 (x = 0.37) Phys.Rev.B, 95(2017)165133 Source remark: Fig shows anti-ferro-insulator (AFI), SC, PM phases , measured by T-sweep, R-sweep resistance and torque method. kink- and dip-temperature in R(T) or R(H) in FIG. Common name (raw) (Fe,Ga)Cl4 Sample form Not supplied Néel temperature (raw) 2.9 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 535–535; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `2fef7368c7639cafd649b58ec8694f0fd327ad4e78da084bc8317feed40141d1` data number · `num` 660 reference number · `refno` PRB095165133 common formula of materials · `name` (Fe,Ga)Cl4 full material name · `fullname` lambda-(BETS)2Fe0.63Ga0.37Cl4 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` 5.05 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` 2.9 figure1 file name · `fig1` OPH660 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Fig shows anti-ferro-insulator (AFI), SC, PM phases , measured by T-sweep, R-sweep resistance and torque method. kink- and dip-temperature in R(T) or R(H) in FIG. figure1 data file name · `f1_filename` OPH660.dat f2 data file name · `f2_filename` — title · `title` Internal field effect on vortex states in the layered organic superconductor lambda-(BETS)2Fe1-xGaxCl4 (x = 0.37) year · `year` 2017 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, 95(2017)165133 author · `author` S. Uji,T. Terashima,T. Konoike,T. Yamaguchi,S. Yasuzuka,A. Kobayashi,B. Zhou sample · `sample` — comments · `comments` —
kappa-(BETS)2FeBr4Row 661 · BETS	Tc 1.5	—	2017 · JPS086014706 Method —
Inspect row 661: properties, remarks and source Anisotropic Field Dependence of the Superconducting Transition in the Magnetic Molecular Superconductor kappa-(BETS)2FeBr4 J.Phys.Soc.Jpn, 86(2017)014706 Source remark: Tn, Tc determined by specific heat C(H,T) measurements. metamagnetic transition at 2 T. Pauli limit = 2.9 T. H-direction is important (anisotropy) Common name (raw) 4-Feb Sample form Not supplied Néel temperature (raw) 2.5 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 536–536; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `347ae4e33058d70cc040fb317b29971c9b90486a5bfaeaca4ede254c47cb9540` data number · `num` 661 reference number · `refno` JPS086014706 common formula of materials · `name` 4-Feb full material name · `fullname` kappa-(BETS)2FeBr4 shape · `shape` — structure · `str` BETS lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 1.5 maximum tc under pressure · `tcmax` — applied pressure for tcmax · `pmax` — Critical pressure/GPa at which Tc can be observed · `pcrit` — tc measurement method · `tcmeth` — alpha in Tc=A*M^(-alpha), isotope effect · `isotope` — isotope element · `isoel` — slope at P=0 in Tc vs P plot · `dtcdp` — lowest temperature for measurement (not superconducting) · `tcn` — Hc1 at 0 K for poly crystal · `hc1zero` — Hc2 at 0 K for poly crystal · `hc2zero` — -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` — penetration depth at 0 K for poly crystal · `penet` — Ginzburg-Landau order parameter · `glpar` — energy gap at 0 K, delta(0) · `gap` — method of measuring energy gap · `gapmeth` — coefficient of electronic specific heat · `gamma` — Debye temperature · `debyet` — Curie temperature · `curiet` — Neel temperature · `neelt` 2.5 figure1 file name · `fig1` OPH661 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` Tn, Tc determined by specific heat C(H,T) measurements. metamagnetic transition at 2 T. Pauli limit = 2.9 T. H-direction is important (anisotropy) figure1 data file name · `f1_filename` OPH661.dat f2 data file name · `f2_filename` — title · `title` Anisotropic Field Dependence of the Superconducting Transition in the Magnetic Molecular Superconductor kappa-(BETS)2FeBr4 year · `year` 2017 keyword · `keyword` — institute · `institute` Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan journal · `journal` J.Phys.Soc.Jpn, 86(2017)014706 author · `author` Shuhei Fukuoka,Satoshi Yamashita,Yasuhiro Nakazawa,Takashi Yamamoto,Hideki Fujiwara sample · `sample` — comments · `comments` —
kappa-(BETS)2FeCl4Row 662 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 662: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: not SC down to 2 K. R(2K)/R(300K) = 2E-4. Space-G = Pnma. Dens = 2.497 g/cm3. For T=10K, a=11.483, b=35.720, c=8.383. Dens = 2.593 g/cm3 Common name (raw) FeCl4 Sample form Not supplied Lattice a (raw) 11.693 Lattice b (raw) 35.945 Lattice c (raw) 8.4914 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 537–537; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `1dba554e3c033305095ab1b2d9b2d816672cdf8c3338bf35409890f6812fb154` data number · `num` 662 reference number · `refno` ACS1180368 common formula of materials · `name` FeCl4 full material name · `fullname` kappa-(BETS)2FeCl4 shape · `shape` — structure · `str` BETS lattice constant a · `lata` 11.693 lattice constant b · `latb` 35.945 lattice constant c · `latc` 8.4914 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` not SC down to 2 K. R(2K)/R(300K) = 2E-4. Space-G = Pnma. Dens = 2.497 g/cm3. For T=10K, a=11.483, b=35.720, c=8.383. Dens = 2.593 g/cm3 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` —
ramda-(BETS)2FeCl4Row 663 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 663: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: not SC down to 2 K. space-G = P1[-]. FIG shows P-dependence of MI transition. d=2.514 g/cm3. For 10K, a=15.890, b=18.378, c=6.531, alpha=98.61, beta=96.67, gamma= 112.05, d = 52.598 g/cm3 Common name (raw) FeCl4 Sample form Not supplied Lattice a (raw) 16.164 Lattice b (raw) 18.538 Lattice c (raw) 6.5928 Lattice α (raw) 98.4 Lattice β (raw) 96.67 Lattice γ (raw) 112.52 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 538–538; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `20ebf35e8a78dd00be296324668adc9fd7ac72a656502f4792c4c44451e8fb52` data number · `num` 663 reference number · `refno` ACS1180368 common formula of materials · `name` FeCl4 full material name · `fullname` ramda-(BETS)2FeCl4 shape · `shape` — structure · `str` BETS lattice constant a · `lata` 16.164 lattice constant b · `latb` 18.538 lattice constant c · `latc` 6.5928 lattice alpha · `alpha` 98.4 lattice beta · `beta` 96.67 lattice gamma · `lgamma` 112.52 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` OTMI663 figure2 filename · `fig2` — figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` not SC down to 2 K. space-G = P1[-]. FIG shows P-dependence of MI transition. d=2.514 g/cm3. For 10K, a=15.890, b=18.378, c=6.531, alpha=98.61, beta=96.67, gamma= 112.05, d = 52.598 g/cm3 figure1 data file name · `f1_filename` OTMI663.dat 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` —
ramda-(BETS)2Fe0.48Ga0.52Cl4Row 664 · BETS	Tc 4.6	—	1996 · ACS1180368 Method —
Inspect row 664: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: Ga-content by EPMA Common name (raw) (Fe,Ga)Cl4 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 539–539; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `3fe36825811b1765d715cf60ecb81cc4f5547b332d50e58b0975415460f84f37` data number · `num` 664 reference number · `refno` ACS1180368 common formula of materials · `name` (Fe,Ga)Cl4 full material name · `fullname` ramda-(BETS)2Fe0.48Ga0.52Cl4 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` 4.6 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` Ga-content by EPMA 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` —
beta-(BDA-TTP)2SbF6Row 665 · BDA-TTP	Tc 7.2	—	2017 · JPS086084704 Method —
Inspect row 665: properties, remarks and source Dimensional Crossover and Its Interplay with In-Plane Anisotropy of Upper Critical Field in beta-(BDA-TTP)2SbF6 J.Phys.Soc.Jpn, 86(2017)084704 Source remark: RRR(R300/R10) > 300. Inter layer distance = 17.6 A. Hc2 defined as R = 0.5Rn. cohere = 133 and 21 A for // and /n/ at 1.5 K. Aniso(Hc2) = 5.8 at 1.5 K. Inplane (ac-plane) anisotropy also measured. Common name (raw) SbF6 Sample form Not supplied Hc2 at 0 K (raw) 12 Coherence length at 0 K (raw) 133 Link to this source row Original NIMS table Field guide, page 9 All 49 original cells and provenance Original physical lines 540–540; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `fcae0d291cd5affa40b5068304b9498fe78f0d774c8ccd37fe6e6e7e94c73f50` data number · `num` 665 reference number · `refno` JPS086084704 common formula of materials · `name` SbF6 full material name · `fullname` beta-(BDA-TTP)2SbF6 shape · `shape` — structure · `str` BDA-TTP lattice constant a · `lata` — lattice constant b · `latb` — lattice constant c · `latc` — lattice alpha · `alpha` — lattice beta · `beta` — lattice gamma · `lgamma` — Tc at pcrit or Tc at atmospheric pressure · `tc` 7.2 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` 12 -slope in Hc2 vs T at Tc for poly crystal · `dhc2dt` — coherence length at 0 K for poly crystal · `cohere` 133 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` OHC665 figure2 filename · `fig2` OCOH665 figure description · `figname` — table file name · `tbl` — table description · `tblname` — comment · `commt` RRR(R300/R10) > 300. Inter layer distance = 17.6 A. Hc2 defined as R = 0.5Rn. cohere = 133 and 21 A for // and /n/ at 1.5 K. Aniso(Hc2) = 5.8 at 1.5 K. Inplane (ac-plane) anisotropy also measured. figure1 data file name · `f1_filename` OHC665.dat f2 data file name · `f2_filename` OCOH665.dat title · `title` Dimensional Crossover and Its Interplay with In-Plane Anisotropy of Upper Critical Field in beta-(BDA-TTP)2SbF6 year · `year` 2017 keyword · `keyword` — institute · `institute` Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan journal · `journal` J.Phys.Soc.Jpn, 86(2017)084704 author · `author` Syuma Yasuzuka,Hiroaki Koga,Yasuhisa Yamamura,Kazuya Saito,Shinya Uji,Taichi Terashima,Hiroki Akutsu,Jun-ichi Yamada sample · `sample` — comments · `comments` —
kappa-(BETS)2CoCl4Row 666 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 666: properties, remarks and source New BETS Conductors with Magnetic Anions (BETS ) = bis(ethylenedithio)tetraselenafulvalene) J.Am.Chem.Soc., 118(1996)368 Source remark: Mettalic for T > 2K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CoCl4, solvent=TCE. Common name (raw) CoCl4 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 541–541; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `77918e89cb1fca43549b6e0e4a574d528454df7a2f327717cd244bf0626c2c0c` data number · `num` 666 reference number · `refno` ACS1180368 common formula of materials · `name` CoCl4 full material name · `fullname` kappa-(BETS)2CoCl4 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` Mettalic for T > 2K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CoCl4, 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)2MnCl4Row 667 · BETS	—	—	1996 · ACS1180368 Method —
Inspect row 667: 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 40 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnCl4, solvent=TCE. Common name (raw) MnCl4 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 542–542; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here. Row SHA-256: `135ebe3d56d550ebfd5203214e0fa1ee7b699bf08f048eede1d394b55fbcf9c7` data number · `num` 667 reference number · `refno` ACS1180368 common formula of materials · `name` MnCl4 full material name · `fullname` (BETS)2MnCl4 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 40 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnCl4, 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` —

Dataset coverage, units and downloads

MDR SuperCon Datasheet Ver.240322, National Institute for Materials Science (NIMS), DOI 10.48505/nims.4487. SCLib preserves all original Organic cells and adds row provenance and a reading interface. Dataset version · CC BY 4.0.

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

The actual source header says Tc at pcrit or atmospheric pressure; the guide abbreviates it as Tc at pcrit. Missing pcrit does not establish ambient pressure. Maximum Tc under pressure; pmax is its associated applied pressure, unlike the oxide/metallic table pmax definition. Lowest measurement temperature for a non-superconducting report, not a Tc value.

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

Full reference JSON JSON SHA-256 Original table bytes

Source file SHA-256: d116848a90d01e48356ed6cf0bb69035fa863a3a559deac1ef188025bdb3b423

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

Source material

Transition values (raw)

Pressure context

Reference / method

kappa-(d-[3:3]BEDT-TTF)2Cu[N(CN)2]BrRow 642 · BEDT-TTF

Tc: 11.9

—

2015 · JPS084064713

Method —

Inspect row 642: properties, remarks and source

Tunneling Spectroscopy in Organic Superconductor kappa-(BEDT-TTF-d[3,3])2Cu[N(CN)2]Br

J.Phys.Soc.Jpn, 84(2015)064713

Source remark: Energy gap measured by STS(tunneling spectroscopy) at 1.2 K on the a-c plane. gap d(0) = 4.0 meV

Common name (raw): Cu[N(CN)2]Br
Sample form: Not supplied
Energy gap at 0 K (raw): 7.8
Gap method: Tunneling (code 1)

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

All 49 original cells and provenance

Original physical lines 523–523; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 7f1145416597d125b3e4ceaf4ef95bbc66ce05ea6b826cdfcdd50a0c91770379

data number · num: 642
reference number · refno: JPS084064713
common formula of materials · name: Cu[N(CN)2]Br
full material name · fullname: kappa-(d-[3:3]BEDT-TTF)2Cu[N(CN)2]Br
shape · shape: —
structure · str: BEDT-TTF
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 11.9
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: 7.8
method of measuring energy gap · gapmeth: 1
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: Energy gap measured by STS(tunneling spectroscopy) at 1.2 K on the a-c plane. gap d(0) = 4.0 meV
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Tunneling Spectroscopy in Organic Superconductor kappa-(BEDT-TTF-d[3,3])2Cu[N(CN)2]Br
year · year: 2015
keyword · keyword: —
institute · institute: Department of Physics, Hokkaido University, Sapporo 060-0810, Japan
journal · journal: J.Phys.Soc.Jpn, 84(2015)064713
author · author: Yuki Oka,Hiroyoshi Nobukane,Noriaki Matsunaga,Kazushige Nomura,Kazuhiro Katono,Koichi Ichimura,Atsushi Kawamoto
sample · sample: —
comments · comments: —

beta''-(BEDT)2SF5CH2CF2SO3Row 643 · BEDT-TTF

Tc: 5.1

Critical pressure, pcrit: 0 GPa

2015 · JPS084094709

Method —

Inspect row 643: properties, remarks and source

In-Plane Anisotropy of Upper Critical Field and Flux-Flow Resistivity in Layered Organic Superconductor beta''-(ET)2SF5CH2CF2SO3

J.Phys.Soc.Jpn, 84(2015)094709

Source remark: Anisotropy and angular dependence of Hc2 were measured. Sample A (Tc=5.1K), B (Tc= 5.2 K)

Common name (raw): SF5CH2CF2SO3
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 524–524; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 3dda349ed6f94d1a16e6a0698e0fd5e67525e663c38749cdeb54f55878efe165

data number · num: 643
reference number · refno: JPS084094709
common formula of materials · name: SF5CH2CF2SO3
full material name · fullname: beta''-(BEDT)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: 5.1
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: 0
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OHC643-1
figure2 filename · fig2: OHC643-2
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Anisotropy and angular dependence of Hc2 were measured. Sample A (Tc=5.1K), B (Tc= 5.2 K)
figure1 data file name · f1_filename: OHC643-1.dat
f2 data file name · f2_filename: OHC643-2.dat
title · title: In-Plane Anisotropy of Upper Critical Field and Flux-Flow Resistivity in Layered Organic Superconductor beta''-(ET)2SF5CH2CF2SO3
year · year: 2015
keyword · keyword: —
institute · institute: Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan
journal · journal: J.Phys.Soc.Jpn, 84(2015)094709
author · author: Syuma Yasuzuka,Shinya Uji,Taichi Terashima,Kaori Sugii,Takayuki Isono,Yoritsugu Iida,John A. Schlueter
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 644 · BETS

Tc: 6

—

2015 · JPS084104709

Method —

Inspect row 644: properties, remarks and source

Vortex Dynamics and Diamagnetic Torque Signals in Two Dimensional Organic Superconductor ramda-(BETS)2GaCl4

J.Phys.Soc.Jpn, 84(2015)104709

Source remark: RRR = 300. R(T) max at 80 K. R-peak appears below Tc(onset) and depends on angle between ac-plane and b*. H//c (defined as R(onset) ) measured .

Common name (raw): GaCl4
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 525–525; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: f1ddc4f6bca87114b1d3458db5610491c67c5d6a2ac7aaa177b2d080ba3216d9

data number · num: 644
reference number · refno: JPS084104709
common formula of materials · name: GaCl4
full material name · fullname: ramda-(BETS)2GaCl4
shape · shape: 3
structure · str: BETS
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 6
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: OHC644
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: RRR = 300. R(T) max at 80 K. R-peak appears below Tc(onset) and depends on angle between ac-plane and b*. H//c (defined as R(onset) ) measured .
figure1 data file name · f1_filename: OHC644.dat
f2 data file name · f2_filename: —
title · title: Vortex Dynamics and Diamagnetic Torque Signals in Two Dimensional Organic Superconductor ramda-(BETS)2GaCl4
year · year: 2015
keyword · keyword: —
institute · institute: National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan
journal · journal: J.Phys.Soc.Jpn, 84(2015)104709
author · author: Shinya Uji,Kouta Kodama,Kaori Sugii1,Taichi Terashima,Takahide Yamaguchi,Nobuyuki Kurita,Satoshi Tsuchiya,Takako Konoike,Motoi Kimata,Akiko Kobayashi,Biao Zhou,Hayao Kobayashi
sample · sample: —
comments · comments: —

K3-piceneRow 645 · picene

Tc: 14

Critical pressure, pcrit: 0 GPa

2015 · PHC5140199

Method —

Inspect row 645: properties, remarks and source

Superconductivity in aromatic hydrocarbons

Physica C, 514(2015)199

Source remark: SC-volume = 3.9% at 2K.

Common name (raw): K3
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 526–526; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: dbc914cb31a06fe4dff4887dc36d7a19c9f810022fff686b653d40e17b8dabab

data number · num: 645
reference number · refno: PHC5140199
common formula of materials · name: K3
full material name · fullname: K3-picene
shape · shape: —
structure · str: picene
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 14
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: SC-volume = 3.9% at 2K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in aromatic hydrocarbons
year · year: 2015
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Physica C, 514(2015)199
author · author: Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu
sample · sample: —
comments · comments: —

K3-[7]phenaceneRow 646 · phenacene

Tc: 11

Critical pressure, pcrit: 0 GPa

2015 · PHC5140199

Method —

Inspect row 646: properties, remarks and source

Superconductivity in aromatic hydrocarbons

Physica C, 514(2015)199

Source remark: SC-volume = 0.1% at 2K.

Common name (raw): K3
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 527–527; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: d1c10c15aea7f6749b87e0e52a90835f34ed9291c76efc39523ea73a1a5081fa

data number · num: 646
reference number · refno: PHC5140199
common formula of materials · name: K3
full material name · fullname: K3-[7]phenacene
shape · shape: —
structure · str: phenacene
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 11
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: SC-volume = 0.1% at 2K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in aromatic hydrocarbons
year · year: 2015
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Physica C, 514(2015)199
author · author: Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu
sample · sample: —
comments · comments: —

Sr1.5-phenanthreneRow 647 · phenanthrene

Tc: 6

Critical pressure, pcrit: 0 GPa

2015 · PHC5140199

Method —

Inspect row 647: properties, remarks and source

Superconductivity in aromatic hydrocarbons

Physica C, 514(2015)199

Source remark: SC-volume = 4% at 2K. Tc(SUS) = 5.3 K.

Common name (raw): Sr1.5
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 528–528; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: c51c37b3a354604513349bed67c03091ee690418323963cb66b24babbc1c681e

data number · num: 647
reference number · refno: PHC5140199
common formula of materials · name: Sr1.5
full material name · fullname: Sr1.5-phenanthrene
shape · shape: —
structure · str: phenanthrene
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 6
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: SC-volume = 4% at 2K. Tc(SUS) = 5.3 K.
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in aromatic hydrocarbons
year · year: 2015
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Physica C, 514(2015)199
author · author: Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu
sample · sample: —
comments · comments: —

Kx-DBPRow 648 · DBP

Tc: 30

Critical pressure, pcrit: 0 GPa

2015 · PHC5140199

Method —

Inspect row 648: properties, remarks and source

Superconductivity in aromatic hydrocarbons

Physica C, 514(2015)199

Source remark: Sample has two-phases: Tc1 = 30K, Tc2 = 7K. , corresponding to different x in Kx-DBP. DBP = dibenzopentacene

Common name (raw): Kx
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 529–529; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 614970b136dbe269aba19311b984fceed66879b5c282026a9d7ca91efc888f8e

data number · num: 648
reference number · refno: PHC5140199
common formula of materials · name: Kx
full material name · fullname: Kx-DBP
shape · shape: —
structure · str: DBP
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: 30
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: Sample has two-phases: Tc1 = 30K, Tc2 = 7K. , corresponding to different x in Kx-DBP. DBP = dibenzopentacene
figure1 data file name · f1_filename: —
f2 data file name · f2_filename: —
title · title: Superconductivity in aromatic hydrocarbons
year · year: 2015
keyword · keyword: —
institute · institute: Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan
journal · journal: Physica C, 514(2015)199
author · author: Yoshihiro Kubozono,Hidenori Goto,Taihei Jabuchi,Takayoshi Yokoya,Takashi Kambe,Yusuke Sakai,Masanari Izumi,Lu Zheng,Shino Hamao,Huyen L.T. Nguyen,Masafumi Sakata,Tomoko Kagayama,Katsuya Shimizu
sample · sample: —
comments · comments: —

beta''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]:PhNO2Row 650 · BEDT-TTF

Tc: 7.5

Critical pressure, pcrit: 0 GPa

2016 · JPS085014601

Method —

Inspect row 650: properties, remarks and source

High-Temperature Charge and Structure Anomalies in (beta)''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]/C6H5NO2

J.Phys.Soc.Jpn, 85(2016)014601

Source remark: There exist the kink at 90 K in C(T) and lattice parameters due to charge ordering. Debye-T = 130 K for T < 50 K fittong.

Common name (raw): [(H3O)Ga(C2O4)3]:PhNO2
Sample form: Not supplied
Lattice a (raw): 10.251
Lattice b (raw): 20.05
Lattice c (raw): 35.19
Lattice β (raw): 92.326
Debye temperature (raw): 130

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

All 49 original cells and provenance

Original physical lines 530–530; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 7eee12f98c70e189f50b8e28952e322b08c4d972c584c84206141a619d538e06

data number · num: 650
reference number · refno: JPS085014601
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: 10.251
lattice constant b · latb: 20.05
lattice constant c · latc: 35.19
lattice alpha · alpha: —
lattice beta · beta: 92.326
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 7.5
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: 130
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OSP650
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: There exist the kink at 90 K in C(T) and lattice parameters due to charge ordering. Debye-T = 130 K for T < 50 K fittong.
figure1 data file name · f1_filename: OSP650.dat
f2 data file name · f2_filename: —
title · title: High-Temperature Charge and Structure Anomalies in (beta)''-(BEDT-TTF)4[(H3O)Ga(C2O4)3]/C6H5NO2
year · year: 2016
keyword · keyword: —
institute · institute: Department of Condensed Matter Physics, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan
journal · journal: J.Phys.Soc.Jpn, 85(2016)014601
author · author: Yoshihiko Ihara,Yosuke Futami,Atsushi Kawamoto
sample · sample: —
comments · comments: —

ramda-(BETS)2FeCl4Row 651 · BETS

—

Critical pressure, pcrit: 0 GPa

2016 · JPS085023601

Method —

Inspect row 651: properties, remarks and source

Effective Field Study of Canted Antiferromagnetic Insulating Phase in Magnetic Organic Conductor ramda-(BETS)2FeCl4 through Specific Heat Measurement

J.Phys.Soc.Jpn, 85(2016)023601

Source remark: H-induced SC. (dC) = C - C(lattice) measured under H//c. Tn obtained from the peak of (dC) for 3 samples for H < 11T

Common name (raw): FeCl4
Sample form: Not supplied
Néel temperature (raw): 8.4

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

All 49 original cells and provenance

Original physical lines 531–531; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: f3a0c194638930330bdd951f46a74200c80ead9f2746c552d77ade6e207eb0ac

data number · num: 651
reference number · refno: JPS085023601
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: —
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: 8.4
figure1 file name · fig1: OPH651
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: H-induced SC. (dC) = C - C(lattice) measured under H//c. Tn obtained from the peak of (dC) for 3 samples for H < 11T
figure1 data file name · f1_filename: OPH651.dat
f2 data file name · f2_filename: —
title · title: Effective Field Study of Canted Antiferromagnetic Insulating Phase in Magnetic Organic Conductor ramda-(BETS)2FeCl4 through Specific Heat Measurement
year · year: 2016
keyword · keyword: —
institute · institute: Department of Physics, Toho University, Funabashi, Chiba 274-8510, Japan
journal · journal: J.Phys.Soc.Jpn, 85(2016)023601
author · author: Kazuo Shimada,Naoya Tajima,Koji Kajita,Yutaka Nishio
sample · sample: —
comments · comments: —

ramda-(BETS)2GaCl4Row 652 · BETS

Tc: 4.8

Critical pressure, pcrit: 0 GPa

2016 · JPS085043705

Method —

Inspect row 652: 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: C = a*T + b*T^3 + c*T^5 + Einstein term(E1, E2): b = 18.2 mJ/mol.K4, c = 0.024 mJ/mol.K6, E1 = 30.6 K, E2 = 46.7 K from data fitting.

Common name (raw): GaCl4
Sample form: Not supplied
Hc2 at 0 K (raw): 3.5
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 532–532; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 6c9acb78cfa620cd6e0dfe13b6934837c88dc249507eeca0ccab68538f8a35ce

data number · num: 652
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: 3.5
-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: 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: C = a*T + b*T^3 + c*T^5 + Einstein term(E1, E2): b = 18.2 mJ/mol.K4, c = 0.024 mJ/mol.K6, E1 = 30.6 K, E2 = 46.7 K from data fitting.
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: —

kappa-(BEDT-TTF)2CF3SO3Row 655 · BEDT-TTF

Tc: 4.7
Maximum Tc: 4.8

Critical pressure, pcrit: 1.1 GPa
At maximum Tc, pmax (raw): 1.3

2016 · PRB094020503

Method —

Inspect row 655: properties, remarks and source

Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice

Phys.Rev.B, 94(2016)020503

Source remark: SC-data at P = 1.45 GPa. Hc2 defined as midpoint. Hc2 depend on current direction

Common name (raw): CF3SO3
Sample form: Single crystal bulk (code 3)
Coherence length at 0 K (raw): 370

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

All 49 original cells and provenance

Original physical lines 533–533; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: f9fe2d33f57d11a82dfe573f5b36cd1564444480d2a1901357daa67b9acdff1a

data number · num: 655
reference number · refno: PRB094020503
common formula of materials · name: CF3SO3
full material name · fullname: kappa-(BEDT-TTF)2CF3SO3
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: 4.7
maximum tc under pressure · tcmax: 4.8
applied pressure for tcmax · pmax: 1.3
Critical pressure/GPa at which Tc can be observed · pcrit: 1.1
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 370
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: OHC655
figure2 filename · fig2: OTC655
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: SC-data at P = 1.45 GPa. Hc2 defined as midpoint. Hc2 depend on current direction
figure1 data file name · f1_filename: OHC655.dat
f2 data file name · f2_filename: OTC655.dat
title · title: Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice
year · year: 2016
keyword · keyword: —
institute · institute: Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan
journal · journal: Phys.Rev.B, 94(2016)020503
author · author: Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito
sample · sample: —
comments · comments: —

kappa-(BEDT-TTF)2CF3SO3Row 656 · BEDT-TTF

Tc: 4.98
Maximum Tc: 4.98

Critical pressure, pcrit: 1.6 GPa
At maximum Tc, pmax (raw): 1.9

2016 · PRB094020503

Method —

Inspect row 656: properties, remarks and source

Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice

Phys.Rev.B, 94(2016)020503

Source remark: Tc for c-axis pressure (strain)

Common name (raw): CF3SO3
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 534–534; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 93a09a2f5fa4bad10fc9581ac35099ed68e0af46d59be758294ccffa302ca501

data number · num: 656
reference number · refno: PRB094020503
common formula of materials · name: CF3SO3
full material name · fullname: kappa-(BEDT-TTF)2CF3SO3
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: 4.98
maximum tc under pressure · tcmax: 4.98
applied pressure for tcmax · pmax: 1.9
Critical pressure/GPa at which Tc can be observed · pcrit: 1.6
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: —
figure1 file name · fig1: OTC656
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Tc for c-axis pressure (strain)
figure1 data file name · f1_filename: OTC656.dat
f2 data file name · f2_filename: —
title · title: Pressure-induced superconductivity in the antiferromagnet kappa-(ET)2CF3SO3 with quasi-one-dimensional triangular spin lattice
year · year: 2016
keyword · keyword: —
institute · institute: Department of Applied Physics, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan
journal · journal: Phys.Rev.B, 94(2016)020503
author · author: Hiroshi Ito,Takayuki Asai,Yasuhiro Shimizu,Hiromi Hayama,Yukihiro Yoshida,Gunzi Saito
sample · sample: —
comments · comments: —

lambda-(BETS)2Fe0.63Ga0.37Cl4Row 660 · BETS

Tc: 5.05

—

2017 · PRB095165133

Method —

Inspect row 660: properties, remarks and source

Internal field effect on vortex states in the layered organic superconductor lambda-(BETS)2Fe1-xGaxCl4 (x = 0.37)

Phys.Rev.B, 95(2017)165133

Source remark: Fig shows anti-ferro-insulator (AFI), SC, PM phases , measured by T-sweep, R-sweep resistance and torque method. kink- and dip-temperature in R(T) or R(H) in FIG.

Common name (raw): (Fe,Ga)Cl4
Sample form: Not supplied
Néel temperature (raw): 2.9

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

All 49 original cells and provenance

Original physical lines 535–535; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 2fef7368c7639cafd649b58ec8694f0fd327ad4e78da084bc8317feed40141d1

data number · num: 660
reference number · refno: PRB095165133
common formula of materials · name: (Fe,Ga)Cl4
full material name · fullname: lambda-(BETS)2Fe0.63Ga0.37Cl4
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: 5.05
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: 2.9
figure1 file name · fig1: OPH660
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Fig shows anti-ferro-insulator (AFI), SC, PM phases , measured by T-sweep, R-sweep resistance and torque method. kink- and dip-temperature in R(T) or R(H) in FIG.
figure1 data file name · f1_filename: OPH660.dat
f2 data file name · f2_filename: —
title · title: Internal field effect on vortex states in the layered organic superconductor lambda-(BETS)2Fe1-xGaxCl4 (x = 0.37)
year · year: 2017
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, 95(2017)165133
author · author: S. Uji,T. Terashima,T. Konoike,T. Yamaguchi,S. Yasuzuka,A. Kobayashi,B. Zhou
sample · sample: —
comments · comments: —

kappa-(BETS)2FeBr4Row 661 · BETS

Tc: 1.5

—

2017 · JPS086014706

Method —

Inspect row 661: properties, remarks and source

Anisotropic Field Dependence of the Superconducting Transition in the Magnetic Molecular Superconductor kappa-(BETS)2FeBr4

J.Phys.Soc.Jpn, 86(2017)014706

Source remark: Tn, Tc determined by specific heat C(H,T) measurements. metamagnetic transition at 2 T. Pauli limit = 2.9 T. H-direction is important (anisotropy)

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

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

All 49 original cells and provenance

Original physical lines 536–536; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 347ae4e33058d70cc040fb317b29971c9b90486a5bfaeaca4ede254c47cb9540

data number · num: 661
reference number · refno: JPS086014706
common formula of materials · name: 4-Feb
full material name · fullname: kappa-(BETS)2FeBr4
shape · shape: —
structure · str: BETS
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 1.5
maximum tc under pressure · tcmax: —
applied pressure for tcmax · pmax: —
Critical pressure/GPa at which Tc can be observed · pcrit: —
tc measurement method · tcmeth: —
alpha in Tc=A*M^(-alpha), isotope effect · isotope: —
isotope element · isoel: —
slope at P=0 in Tc vs P plot · dtcdp: —
lowest temperature for measurement (not superconducting) · tcn: —
Hc1 at 0 K for poly crystal · hc1zero: —
Hc2 at 0 K for poly crystal · hc2zero: —
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: —
penetration depth at 0 K for poly crystal · penet: —
Ginzburg-Landau order parameter · glpar: —
energy gap at 0 K, delta(0) · gap: —
method of measuring energy gap · gapmeth: —
coefficient of electronic specific heat · gamma: —
Debye temperature · debyet: —
Curie temperature · curiet: —
Neel temperature · neelt: 2.5
figure1 file name · fig1: OPH661
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: Tn, Tc determined by specific heat C(H,T) measurements. metamagnetic transition at 2 T. Pauli limit = 2.9 T. H-direction is important (anisotropy)
figure1 data file name · f1_filename: OPH661.dat
f2 data file name · f2_filename: —
title · title: Anisotropic Field Dependence of the Superconducting Transition in the Magnetic Molecular Superconductor kappa-(BETS)2FeBr4
year · year: 2017
keyword · keyword: —
institute · institute: Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan
journal · journal: J.Phys.Soc.Jpn, 86(2017)014706
author · author: Shuhei Fukuoka,Satoshi Yamashita,Yasuhiro Nakazawa,Takashi Yamamoto,Hideki Fujiwara
sample · sample: —
comments · comments: —

kappa-(BETS)2FeCl4Row 662 · BETS

—

1996 · ACS1180368

Method —

Inspect row 662: properties, remarks and source

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

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

Source remark: not SC down to 2 K. R(2K)/R(300K) = 2E-4. Space-G = Pnma. Dens = 2.497 g/cm3. For T=10K, a=11.483, b=35.720, c=8.383. Dens = 2.593 g/cm3

Common name (raw): FeCl4
Sample form: Not supplied
Lattice a (raw): 11.693
Lattice b (raw): 35.945
Lattice c (raw): 8.4914

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

All 49 original cells and provenance

Original physical lines 537–537; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 1dba554e3c033305095ab1b2d9b2d816672cdf8c3338bf35409890f6812fb154

data number · num: 662
reference number · refno: ACS1180368
common formula of materials · name: FeCl4
full material name · fullname: kappa-(BETS)2FeCl4
shape · shape: —
structure · str: BETS
lattice constant a · lata: 11.693
lattice constant b · latb: 35.945
lattice constant c · latc: 8.4914
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: not SC down to 2 K. R(2K)/R(300K) = 2E-4. Space-G = Pnma. Dens = 2.497 g/cm3. For T=10K, a=11.483, b=35.720, c=8.383. Dens = 2.593 g/cm3
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: —

ramda-(BETS)2FeCl4Row 663 · BETS

—

1996 · ACS1180368

Method —

Inspect row 663: properties, remarks and source

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

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

Source remark: not SC down to 2 K. space-G = P1[-]. FIG shows P-dependence of MI transition. d=2.514 g/cm3. For 10K, a=15.890, b=18.378, c=6.531, alpha=98.61, beta=96.67, gamma= 112.05, d = 52.598 g/cm3

Common name (raw): FeCl4
Sample form: Not supplied
Lattice a (raw): 16.164
Lattice b (raw): 18.538
Lattice c (raw): 6.5928
Lattice α (raw): 98.4
Lattice β (raw): 96.67
Lattice γ (raw): 112.52

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All 49 original cells and provenance

Original physical lines 538–538; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 20ebf35e8a78dd00be296324668adc9fd7ac72a656502f4792c4c44451e8fb52

data number · num: 663
reference number · refno: ACS1180368
common formula of materials · name: FeCl4
full material name · fullname: ramda-(BETS)2FeCl4
shape · shape: —
structure · str: BETS
lattice constant a · lata: 16.164
lattice constant b · latb: 18.538
lattice constant c · latc: 6.5928
lattice alpha · alpha: 98.4
lattice beta · beta: 96.67
lattice gamma · lgamma: 112.52
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: OTMI663
figure2 filename · fig2: —
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: not SC down to 2 K. space-G = P1[-]. FIG shows P-dependence of MI transition. d=2.514 g/cm3. For 10K, a=15.890, b=18.378, c=6.531, alpha=98.61, beta=96.67, gamma= 112.05, d = 52.598 g/cm3
figure1 data file name · f1_filename: OTMI663.dat
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: —

ramda-(BETS)2Fe0.48Ga0.52Cl4Row 664 · BETS

Tc: 4.6

—

1996 · ACS1180368

Method —

Inspect row 664: properties, remarks and source

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

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

Source remark: Ga-content by EPMA

Common name (raw): (Fe,Ga)Cl4
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 539–539; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 3fe36825811b1765d715cf60ecb81cc4f5547b332d50e58b0975415460f84f37

data number · num: 664
reference number · refno: ACS1180368
common formula of materials · name: (Fe,Ga)Cl4
full material name · fullname: ramda-(BETS)2Fe0.48Ga0.52Cl4
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: 4.6
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: Ga-content by EPMA
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: —

beta-(BDA-TTP)2SbF6Row 665 · BDA-TTP

Tc: 7.2

—

2017 · JPS086084704

Method —

Inspect row 665: properties, remarks and source

Dimensional Crossover and Its Interplay with In-Plane Anisotropy of Upper Critical Field in beta-(BDA-TTP)2SbF6

J.Phys.Soc.Jpn, 86(2017)084704

Source remark: RRR(R300/R10) > 300. Inter layer distance = 17.6 A. Hc2 defined as R = 0.5Rn. cohere = 133 and 21 A for // and /n/ at 1.5 K. Aniso(Hc2) = 5.8 at 1.5 K. Inplane (ac-plane) anisotropy also measured.

Common name (raw): SbF6
Sample form: Not supplied
Hc2 at 0 K (raw): 12
Coherence length at 0 K (raw): 133

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All 49 original cells and provenance

Original physical lines 540–540; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: fcae0d291cd5affa40b5068304b9498fe78f0d774c8ccd37fe6e6e7e94c73f50

data number · num: 665
reference number · refno: JPS086084704
common formula of materials · name: SbF6
full material name · fullname: beta-(BDA-TTP)2SbF6
shape · shape: —
structure · str: BDA-TTP
lattice constant a · lata: —
lattice constant b · latb: —
lattice constant c · latc: —
lattice alpha · alpha: —
lattice beta · beta: —
lattice gamma · lgamma: —
Tc at pcrit or Tc at atmospheric pressure · tc: 7.2
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: 12
-slope in Hc2 vs T at Tc for poly crystal · dhc2dt: —
coherence length at 0 K for poly crystal · cohere: 133
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: OHC665
figure2 filename · fig2: OCOH665
figure description · figname: —
table file name · tbl: —
table description · tblname: —
comment · commt: RRR(R300/R10) > 300. Inter layer distance = 17.6 A. Hc2 defined as R = 0.5Rn. cohere = 133 and 21 A for // and /n/ at 1.5 K. Aniso(Hc2) = 5.8 at 1.5 K. Inplane (ac-plane) anisotropy also measured.
figure1 data file name · f1_filename: OHC665.dat
f2 data file name · f2_filename: OCOH665.dat
title · title: Dimensional Crossover and Its Interplay with In-Plane Anisotropy of Upper Critical Field in beta-(BDA-TTP)2SbF6
year · year: 2017
keyword · keyword: —
institute · institute: Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan
journal · journal: J.Phys.Soc.Jpn, 86(2017)084704
author · author: Syuma Yasuzuka,Hiroaki Koga,Yasuhisa Yamamura,Kazuya Saito,Shinya Uji,Taichi Terashima,Hiroki Akutsu,Jun-ichi Yamada
sample · sample: —
comments · comments: —

kappa-(BETS)2CoCl4Row 666 · BETS

—

1996 · ACS1180368

Method —

Inspect row 666: properties, remarks and source

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

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

Source remark: Mettalic for T > 2K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CoCl4, solvent=TCE.

Common name (raw): CoCl4
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 541–541; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 77918e89cb1fca43549b6e0e4a574d528454df7a2f327717cd244bf0626c2c0c

data number · num: 666
reference number · refno: ACS1180368
common formula of materials · name: CoCl4
full material name · fullname: kappa-(BETS)2CoCl4
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: Mettalic for T > 2K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)CoCl4, 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)2MnCl4Row 667 · BETS

—

1996 · ACS1180368

Method —

Inspect row 667: 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 40 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnCl4, solvent=TCE.

Common name (raw): MnCl4
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 542–542; blank cells are preserved. Linked figure/table filenames are source metadata; their files have not been inspected here.

Row SHA-256: 135ebe3d56d550ebfd5203214e0fa1ee7b699bf08f048eede1d394b55fbcf9c7

data number · num: 667
reference number · refno: ACS1180368
common formula of materials · name: MnCl4
full material name · fullname: (BETS)2MnCl4
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 40 K. Prepared using electrolyte= ([solvent(with 10%ethanol)N]n)MnCl4, 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: —