{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1360004239480737280.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.3390/cryst2031034"}},{"identifier":{"@type":"URI","@value":"https://www.mdpi.com/2073-4352/2/3/1034/pdf"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Magnetic and Electric Properties of Organic Conductors Probed by 13C-NMR Using Selective-Site Substituted Molecules"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Quasi-One and quasi-two dimensional organic conductors consisting of TTF derivatives such as BEDT-TTF (bis-(ethylene-dithio)-tetra-thia-fulvalene) and TMTCF (C = S; TMTTF: tetra-methyl-tetra-thia-fulvalene, C = Se; TMTSF: tetra-methyl-tetra-selena-fulvalene) have been well investigated in condensed matter physics because of interest in the emerging electric and magnetic properties, such as the spin density wave, charge order, superconductivity, anti-ferromagnetism, and so on. To probe the electronic state, nuclear magnetic resonance (NMR) is one of the most powerful tools as the microscopic magnetometer. A number of 13C-NMR studies have been performed of the double-site central 13C=13C bond substituted molecules. However, problems with the coupled spin system of 13C=13C complicated the interpretation for observations on NMR. Therefore, single-site 13C-enriched molecules are desired. We summarize the problem of Pake doublet and the preparation of the single-site 13C-susbstituted BEDT-TTF and TMTCF molecules. We also demonstrate the superiority of 13C-NMR of the single-site 13C-susbstituted molecule utilizing the hyperfine coupling tensor.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004239480737153","@type":"Researcher","foaf:name":[{"@value":"Shinji Hirose"}],"jpcoar:affiliationName":[{"@value":"Department of Condensed Matter Physics, Hokkaido University, Kita-ku Sapporo, Hokkaido 060-0810, Japan"}]},{"@id":"https://cir.nii.ac.jp/crid/1380004239480737538","@type":"Researcher","foaf:name":[{"@value":"Masaki Misawa"}],"jpcoar:affiliationName":[{"@value":"Department of Condensed Matter Physics, Hokkaido University, Kita-ku Sapporo, Hokkaido 060-0810, Japan"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801188080128","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"60251691"},{"@type":"NRID","@value":"1000060251691"},{"@type":"NRID","@value":"9000003213140"},{"@type":"NRID","@value":"9000401887343"},{"@type":"NRID","@value":"9000415111753"},{"@type":"NRID","@value":"9000003726022"},{"@type":"NRID","@value":"9000401895402"},{"@type":"NRID","@value":"9000412163246"},{"@type":"NRID","@value":"9000016926858"},{"@type":"NRID","@value":"9000241659606"},{"@type":"NRID","@value":"9000256010350"},{"@type":"NRID","@value":"9000237782915"},{"@type":"NRID","@value":"9000020625653"},{"@type":"NRID","@value":"9000270140879"},{"@type":"NRID","@value":"9000021858764"},{"@type":"NRID","@value":"9000000239464"},{"@type":"NRID","@value":"9000045808174"},{"@type":"NRID","@value":"9000251869979"},{"@type":"NRID","@value":"9000021782197"},{"@type":"NRID","@value":"9000415057107"},{"@type":"NRID","@value":"9000257701519"},{"@type":"NRID","@value":"9000414839104"},{"@type":"NRID","@value":"9000021862636"},{"@type":"NRID","@value":"9000401975996"},{"@type":"NRID","@value":"9000005619523"},{"@type":"NRID","@value":"9000021824226"},{"@type":"NRID","@value":"9000402063137"},{"@type":"NRID","@value":"9000256007344"},{"@type":"NRID","@value":"9000258201567"},{"@type":"NRID","@value":"9000389944869"},{"@type":"NRID","@value":"9000403148338"},{"@type":"NRID","@value":"9000370253577"},{"@type":"NRID","@value":"9000242838752"},{"@type":"NRID","@value":"9000303985481"},{"@type":"NRID","@value":"9000401965879"},{"@type":"NRID","@value":"9000409792270"},{"@type":"NRID","@value":"9000240217720"},{"@type":"NRID","@value":"9000020606289"},{"@type":"NRID","@value":"9000411543616"},{"@type":"NRID","@value":"9000406225592"},{"@type":"NRID","@value":"9000401974736"},{"@type":"NRID","@value":"9000415094514"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/atkawa"}],"foaf:name":[{"@value":"Atsushi Kawamoto"}],"jpcoar:affiliationName":[{"@value":"Department of Condensed Matter Physics, Hokkaido University, Kita-ku Sapporo, Hokkaido 060-0810, Japan"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"20734352"}],"prism:publicationName":[{"@value":"Crystals"}],"dc:publisher":[{"@value":"MDPI AG"}],"prism:publicationDate":"2012-07-27","prism:volume":"2","prism:number":"3","prism:startingPage":"1034","prism:endingPage":"1057"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://creativecommons.org/licenses/by/3.0/"],"url":[{"@id":"https://www.mdpi.com/2073-4352/2/3/1034/pdf"}],"createdAt":"2012-07-28","modifiedAt":"2025-10-11","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Crystallography","dc:title":"Crystallography"},{"@id":"https://cir.nii.ac.jp/all?q=QD901-999","dc:title":"QD901-999"},{"@id":"https://cir.nii.ac.jp/all?q=TMTTF","dc:title":"TMTTF"},{"@id":"https://cir.nii.ac.jp/all?q=TMTSF","dc:title":"TMTSF"},{"@id":"https://cir.nii.ac.jp/all?q=Pake%20doublet","dc:title":"Pake doublet"},{"@id":"https://cir.nii.ac.jp/all?q=hyperfine%20coupling%20tensor","dc:title":"hyperfine coupling tensor"},{"@id":"https://cir.nii.ac.jp/all?q=13C-NMR","dc:title":"13C-NMR"},{"@id":"https://cir.nii.ac.jp/all?q=BEDT-TTF","dc:title":"BEDT-TTF"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040282257184779776","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"24540353"},{"@type":"JGN","@value":"JP24540353"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-24540353/"}],"notation":[{"@language":"ja","@value":"電荷不均化を持つ新奇有機超伝導体の超伝導の対称性とＦＦＬＯ状態の探索"},{"@language":"en","@value":"Investigation of the symmetry of superconducting gap and the FFLO state in a novel organic superconductor with the charge disproportionation"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001337818838272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"ja","@value":"Antiferromagnetic Fluctuations in the Organic Superconductor kappa-(BEDT-TTF)(2)Cu(NCS)(2) under Pressure"},{"@language":"en","@value":"Antiferromagnetic Fluctuations in the Organic Superconductor κ-(BEDT-TTF)2Cu(NCS)2 under Pressure"},{"@value":"Antiferromagnetic Fluctuations in the Organic Superconductor<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>κ</mml:mi><mml:mtext mathvariant=\"normal\">−</mml:mtext><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext mathvariant=\"normal\">−</mml:mtext><mml:mi>TTF</mml:mi><mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mn>2</mml:mn></mml:msub><mml:mi>Cu</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>NCS</mml:mi><mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mn>2</mml:mn></mml:msub></mml:math>under Pressure"}]},{"@id":"https://cir.nii.ac.jp/crid/1050306506459195392","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Nonuniform site-charge distribution and fluctuations of charge order 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display=\"inline\"><mml:mrow><mml:msup><mml:mi>α</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>BEDT-TTF</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mtext>IBr</mml:mtext></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>"},{"@value":"13C NMR study on the charge-ordering salt α'-(BEDT-TTF)2IBr2"},{"@value":"13C NMR study on the charge-ordering salt α′-(BEDT-TTF)2IBr2"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002217814662528","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Charge ordering and antiferromagnetism in (TMTTF)<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub></mml:math>SbF<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mrow/><mml:mn>6</mml:mn></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002219104628224","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Magnetic Properties of TTF-Type Charge Transfer Salts in the Mott Insulator Regime"}]},{"@id":"https://cir.nii.ac.jp/crid/1360003449881910016","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Antiferromagnetic Ordering in Organic Conductor λ-(BEDT-TTF)<sub>2</sub>GaCl<sub>4</sub> Probed by <sup>13</sup>C NMR"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011143496606208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Antiferromagnetic phase in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mi>β</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>BEDT-TTF</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mtext>ICl</mml:mtext></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>under pressure as seen via<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mtext>C</mml:mtext><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>NMR"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011143713578752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charge Ordering in the TMTTF Family of Molecular Conductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011143996496128","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charge ordering in a quasi-two-dimensional organic conductor"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709967442560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Evidence of antiferromagnetic fluctuation in the unconventional superconductor \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>λ</mml:mi></mml:math>\n-(BETS)\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>GaCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>\n by \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math>\n NMR"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619051731840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:math>NMR study of nesting instability in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">α</mml:mi><mml:mo>−</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">B</mml:mi><mml:mi mathvariant=\"normal\">E</mml:mi><mml:mi mathvariant=\"normal\">D</mml:mi><mml:mi mathvariant=\"normal\">T</mml:mi><mml:mo>−</mml:mo><mml:mi mathvariant=\"normal\">T</mml:mi><mml:mi mathvariant=\"normal\">T</mml:mi><mml:mi mathvariant=\"normal\">F</mml:mi><mml:mo>)</mml:mo><mml:mn/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">RbHg</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">SCN</mml:mi><mml:mo>)</mml:mo><mml:mn/></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619085367296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>NMR studies of the normal and superconducting states of the organic superconductor κ-(ET<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu[N(CN<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]Br"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619271584640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>NMR line-shape studies of the organic superconductor κ-(ET<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu[N(CN<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]Br"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619784934912","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Pairing due to Spin Fluctuations in Layered Organic Superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620649305088","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Correlation between non-Fermi-liquid behavior and antiferromagnetic fluctuations in (TMTSF)<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>PF<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>observed using<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>-NMR spectroscopy"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184944832768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Coupling of molecular motion and electronic state in the organic molecular dimer Mott insulator \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msup><mml:mi>β</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:math>\n-(BEDT-TTF)\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>ICl</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094059181568","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Indications of unconventional superconductivity in doped and undoped triangular antiferromagnets"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094141304704","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Double-pulse nuclear-resonance transients in solids"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095812597504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Similarities Between Organic and Cuprate Superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096331880704","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Synthesis of Unsymmetrical Tetrathiafulvalene Derivatives via Me<sub>3</sub>Al-Promoted Reactions of Organotin Compounds with Esters"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659923014016","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Site-specific \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math>\n NMR study on the locally distorted triangular lattice of the organic conductor \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>κ</mml:mi><mml:mo>−</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mo>−</mml:mo><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Cu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>CN</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569325748224","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Magnetic Properties of the Organic Conductor<i>bis</i>-Tetramethyltetraselenafulvalene Hexafluorophosphate [<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mn/><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">TMTSF</mml:mi><mml:mo>)</mml:mo><mml:mn/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>P<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">F</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]: A New Phase Transition"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861705580603392","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Relationship between electronic inhomogeneity and bandwidth in the organic conductor \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi>κ</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext>−</mml:mtext><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mi>Cu</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">N</mml:mi><mml:mo>(</mml:mo><mml:mi>CN</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mi mathvariant=\"normal\">I</mml:mi></mml:mrow></mml:math>\n studied by \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math>\n NMR spectroscopy"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137044471952000","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Wigner Crystal Type of Charge Ordering in an Organic Conductor with a Quarter-Filled Band:<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" 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(BEDT-TTF)Cu[N(CN)2]2"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994655589632","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Zero-Pressure Organic Superconductor: Di-(Tetramethyltetraselenafulvalenium)-Perchlorate [<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mn/><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">TMTSF</mml:mi><mml:mo>)</mml:mo><mml:mn/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cl<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995069278336","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Superconductivity Mediated by Charge Fluctuations in Layered Molecular 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mathvariant=\"normal\">Se</mml:mi></mml:math>Knight shifts for triplet superconductivity in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">TMTSF</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">PF</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943677123328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Electron correlation, metal-insulator transition and superconductivity in quasi-2D organic systems, (ET)2X"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943765554432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Glass transition in the spin-density wave phase of (TMTSF<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">PF</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262946038469376","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charge disproportionation and dynamics in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>θ</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext>−</mml:mtext><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mi mathvariant=\"normal\">Cs</mml:mi><mml:mi mathvariant=\"normal\">Zn</mml:mi><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">S</mml:mi><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mi mathvariant=\"normal\">N</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825893817311360","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Competition and coexistence of bond and charge orders in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">TMTTF</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">AsF</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369910026624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Examination of the Charge-Sensitive Vibrational Modes in Bis(ethylenedithio)tetrathiafulvalene"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370659332992","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Synthesis, Structure and Physical Properties of a Two-Dimensional Organic Metal, Di[bis(ethylenedithiolo)tetrathiofulvalene] triiodide, (BEDT-TTF)<sup>+</sup><sub>2</sub>I<sup>−</sup><sub>3</sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843535362304","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"NMR in Commensurate and Incommensurate Spin Density Waves"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843715995136","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Electron correlation in the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>κ</mml:mi></mml:math>-phase family of BEDT-TTF compounds studied by<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>NMR, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843880648448","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Pressure-temperature phase diagram, inverse isotope effect, and superconductivity in excess of 13 K in κ-(BEDT-TTF<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu[N(CN<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]Cl, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844553501696","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Systematic study of the electronic state in θ-type BEDT-TTF organic conductors by changing the electronic correlation"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319353614720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Synthesis of the organic conductor tetramethyltetraselenofulvalenium 7,7,8,8-tetracyano-p-quinodimethanide (TMTSF–TCNQ)[4,4′,5,5′-tetramethyl-Δ<sup>2,2′</sup>-bis-1,3-diselenolium 3,6-bis-(dicyanomethylene)cyclohexadienide]"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319359978624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Low-frequency dynamics of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>κ</mml:mi></mml:mrow></mml:math>-(BEDT-TTF)<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu(NCS)<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>observed by<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>NMR"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319963705344","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Ambient-pressure superconductivity at the highest temperature (5 K) observed in an organic system: .beta.-(BEDT-TTF)2AuI2"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320030061312","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Resistivity studies under hydrostatic pressure on a low-resistance variant of the quasi-two-dimensional organic superconductor<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>κ</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext>−</mml:mtext><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mi mathvariant=\"normal\">Cu</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant=\"normal\">N</mml:mi><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant=\"normal\">C</mml:mi><mml:mi mathvariant=\"normal\">N</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mi mathvariant=\"normal\">Br</mml:mi></mml:mrow></mml:math>: Search for intrinsic scattering contributions"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320596159872","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Synthesis of the highly conducting organic salt: tetramethyltetrathiofulvalenium - tetracyano--quinodimethanide"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793186486016","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charge ordering in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>θ</mml:mi><mml:mo>−</mml:mo><mml:mo>(</mml:mo><mml:mi 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