{"@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/1363670318937430528.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1126/science.235.4793.1196"}},{"identifier":{"@type":"URI","@value":"https://www.science.org/doi/pdf/10.1126/science.235.4793.1196"}}],"dc:title":[{"@value":"The Resonating Valence Bond State in La\n            <sub>2</sub>\n            CuO\n            <sub>4</sub>\n            and Superconductivity"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>\n            The oxide superconductors, particularly those recently discovered that are based on La\n            <jats:sub>2</jats:sub>\n            CuO\n            <jats:sub>4</jats:sub>\n            , have a set of peculiarities that suggest a common, unique mechanism: they tend in every case to occur near a metal-insulator transition into an odd-electron insulator with peculiar magnetic properties. This insulating phase is proposed to be the long-sought \"resonating-valence-bond\" state or \"quantum spin liquid\" hypothesized in 1973. This insulating magnetic phase is favored by low spin, low dimensionality, and magnetic frustration. The preexisting magnetic singlet pairs of the insulating state become charged superconducting pairs when the insulator is doped sufficiently strongly. The mechanism for superconductivity is hence predominantly electronic and magnetic, although weak phonon interactions may favor the state. Many unusual properties are predicted, especially of the insulating state.\n          </jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004236238519052","@type":"Researcher","foaf:name":[{"@value":"P. W. Anderson"}],"jpcoar:affiliationName":[{"@value":"Department of Physics, Princeton University, Princeton, NJ 08544."}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00368075"},{"@type":"EISSN","@value":"10959203"},{"@type":"PISSN","@value":"http://id.crossref.org/issn/00368075"},{"@type":"PISSN","@value":"https://id.crossref.org/issn/00368075"}],"prism:publicationName":[{"@value":"Science"}],"dc:publisher":[{"@value":"American Association for the Advancement of Science (AAAS)"}],"prism:publicationDate":"1987-03-06","prism:volume":"235","prism:number":"4793","prism:startingPage":"1196","prism:endingPage":"1198"},"reviewed":"false","url":[{"@id":"https://www.science.org/doi/pdf/10.1126/science.235.4793.1196"}],"createdAt":"2006-10-05","modifiedAt":"2024-01-12","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050019822484590208","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Proximate Tomonaga-Luttinger liquid in an anisotropic Kitaev-Gamma model"}]},{"@id":"https://cir.nii.ac.jp/crid/1050569302453360640","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Effects of uniaxial pressure on the spin ice Ho2Ti2O7"},{"@value":"Effects of uniaxial pressure on the spin ice \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mi>Ho</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Ti</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mn>7</mml:mn></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1050587981432644096","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Resonating-Valence-Bond Liquid in Low Dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1050587981434535808","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Residual Entropy of the Mott Insulator with No Symmetry Broken"}]},{"@id":"https://cir.nii.ac.jp/crid/1050588589886650240","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Triangular lattice atomic layer of Sn(1 × 1) at graphene/SiC(0001) interface"}]},{"@id":"https://cir.nii.ac.jp/crid/1050588667319522048","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Magnon spectra of cuprates beyond spin wave theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050856995323724032","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Direct Observation of the Quantum Phase Transition of SrCu2(BO3)(2) by High-Pressure and Terahertz Electron Spin Resonance"},{"@value":"Direct Observation of the Quantum Phase Transition of SrCu<sub>2</sub>(BO<sub>3</sub>)<sub>2</sub> by High-Pressure and Terahertz Electron Spin Resonance"}]},{"@id":"https://cir.nii.ac.jp/crid/1050864247416110464","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Geometric, electronic and spin structures of the CaMn4O5 catalyst for water oxidation in oxygen-evolving photosystem II. 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