{"@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/1363670319708973184.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/s0921-4534(01)00176-9"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0921453401001769?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0921453401001769?httpAccept=text/plain"}},{"identifier":{"@type":"NAID","@value":"30003623263"}}],"dc:title":[{"@value":"Bandwidth and band filling control in organic conductors"}],"description":[{"notation":[{"@value":"Abstract   In order to search and clarify the mechanism of organic superconductors, it is of importance to control the electronic state systematically and elucidate the electronic phase diagram. In organic conductors,  bandwidth control  is usually applied to change the electronic states from insulating, superconducting, to metallic state. By the chemical bandwidth control with introducing Se atoms, the antiferromagnetic insulator, λ-ET 2 GaCl 4 , newly prepared, shifts to the semiconductor, λ-(us-BEDT-STF) 2 GaCl 4 , and superconductor, λ-BETS 2 GaCl 4 . It is clarified that λ-type organic superconductor has been obtained by the  chemical bandwidth control  of the antiferromagnetic insulator. In this paper, our recent successful results of  band filling control  in organic conductors are also reported."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1581417126105180544","@type":"Researcher","foaf:name":[{"@value":"H. Mori"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973312","@type":"Researcher","foaf:name":[{"@value":"T. Okano"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973184","@type":"Researcher","foaf:name":[{"@value":"M. Kamiya"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973185","@type":"Researcher","foaf:name":[{"@value":"M. Haemori"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973313","@type":"Researcher","foaf:name":[{"@value":"H. Suzuki"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973188","@type":"Researcher","foaf:name":[{"@value":"S. Tanaka"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973190","@type":"Researcher","foaf:name":[{"@value":"Y. Nishio"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973187","@type":"Researcher","foaf:name":[{"@value":"K. Kajita"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670319708973186","@type":"Researcher","foaf:name":[{"@value":"H. Moriyama"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"09214534"}],"prism:publicationName":[{"@value":"Physica C: Superconductivity"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2001-09","prism:volume":"357-360","prism:startingPage":"103","prism:endingPage":"107"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S0921453401001769?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S0921453401001769?httpAccept=text/plain"}],"createdAt":"2002-10-31","modifiedAt":"2019-04-25","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050292859826559872","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"ja","@value":"Antiferromagnetic ordering of organic Mott insulator λ-(BEDSe-TTF)2GaCl4"},{"@value":"Antiferromagnetic ordering of organic Mott insulator 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xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi>λ</mml:mi></mml:mrow></mml:math>\n-type organic conductors studied by \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Ga</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>69</mml:mn><mml:mo>,</mml:mo><mml:mn>71</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>\n-NMR spectroscopy"}]},{"@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/1360003449882036992","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Multistep Development of the Hyperfine Fields in λ-(BEDT-STF)<sub>2</sub>FeCl<sub>4</sub> Studied by Mössbauer Spectroscopy"}]},{"@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/1360568469972247936","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Spin-density wave 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