{"@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/1390001204187527936.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1143/jpsj.72.3189"}},{"identifier":{"@type":"BIBCODE","@value":"2003JPSJ...72.3189F"}},{"identifier":{"@type":"NDL_BIB_ID","@value":"6789471"}},{"identifier":{"@type":"URI","@value":"http://id.ndl.go.jp/bib/6789471"}},{"identifier":{"@type":"URI","@value":"https://ndlsearch.ndl.go.jp/books/R000000004-I6789471"}},{"identifier":{"@type":"URI","@value":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.72.3189"}},{"identifier":{"@type":"NAID","@value":"210000104602"}},{"identifier":{"@type":"NAID","@value":"110001954365"}},{"identifier":{"@type":"NAID","@value":"130004538358"}}],"dc:title":[{"@language":"en","@value":"Application of Doniach Diagram on Valence Transition in EuCu2(SixGe1-x)2"},{"@value":"Application of Doniach Diagram on Valence Transition in EuCu<sub>2</sub>(Si<sub><i>x</i></sub>Ge<sub>1-<i>x</i></sub>)<sub>2</sub>"}],"dc:language":"en","description":[{"type":"abstract","notation":[{"@language":"en","@value":"To investigate the valence transition of Eu in the pseudo-binary compounds series, EuCu<SUB>2</SUB>(Si<I><SUB>x</SUB></I>Ge<SUB>1−<I>x</I></SUB>)<SUB>2</SUB>, measurements of the lattice constants, the X-ray absorption spectroscopy (XAS), the magnetic susceptibility, χ, the electric resistivity, ρ, the thermoelectric power, <I>S</I>, and the specific heat, <I>C</I>, have been carried out. The antiferromagnetic order for the samples with 0≤<I>x</I>≤0.50, the temperature-induced valence transition for the samples with 0.68≤<I>x</I>≤1.0 and the state with a high electronic specific heat coefficient for the samples having the intermediate range of <I>x</I> of the above two were observed. The plotting of the Néel temperature, <I>T</I><SUB>N</SUB>, and of the valence transition temperature, <I>T</I><SUB>V</SUB>, as the function of <I>x</I> is found to resemble very well to the Doniach diagram, giving an evidence of the competition of the two interactions, the one for the valence transition, the other for the magnetic order. The observation of the sign change of <I>S</I> near to the temperature <I>T</I><SUB>V</SUB> is found to be a new feature of Eu compounds."}],"abstractLicenseFlag":"disallow"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1410001204187528068","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197294"},{"@type":"NRID","@value":"9000003248724"},{"@type":"NRID","@value":"9000401891231"}],"foaf:name":[{"@language":"en","@value":"Goto Tsuneaki"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Institute for Solid State Physics, University of Tokyo"}]},{"@id":"https://cir.nii.ac.jp/crid/1420845751165004800","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"70361756"},{"@type":"NRID","@value":"1000070361756"},{"@type":"ORCID","@value":"0000-0001-9586-6584"},{"@type":"NRID","@value":"9000016408192"},{"@type":"NRID","@value":"9000259311136"},{"@type":"NRID","@value":"9000401890842"},{"@type":"NRID","@value":"9000384269319"},{"@type":"NRID","@value":"9000384269283"},{"@type":"NRID","@value":"9000402283832"},{"@type":"NRID","@value":"9000402070098"},{"@type":"NRID","@value":"9000257792131"},{"@type":"NRID","@value":"9000258197295"},{"@type":"NRID","@value":"9000003248725"},{"@type":"NRID","@value":"9000257794450"},{"@type":"NRID","@value":"9000411103199"},{"@type":"NRID","@value":"9000389942793"},{"@type":"NRID","@value":"9000401891232"},{"@type":"NRID","@value":"9000384269327"},{"@type":"NRID","@value":"9000406018483"},{"@type":"NRID","@value":"9000258197169"},{"@type":"NRID","@value":"9000001624210"},{"@type":"NRID","@value":"9000384269294"},{"@type":"NRID","@value":"9000402069689"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/TYamamoto1213"}],"foaf:name":[{"@language":"en","@value":"Yamamoto Takashi"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Chemical Resources Laboratory, Tokyo Institute of Technology"}]},{"@id":"https://cir.nii.ac.jp/crid/1410001204187528064","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197293"},{"@type":"NRID","@value":"9000003248723"},{"@type":"NRID","@value":"9000401891230"}],"foaf:name":[{"@language":"en","@value":"Ishikawa Fumihiro"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Institute for Solid State Physics, University of Tokyo"}]},{"@id":"https://cir.nii.ac.jp/crid/1410001204187527936","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197289"},{"@type":"NRID","@value":"9000003248717"},{"@type":"NRID","@value":"9000401891226"}],"foaf:name":[{"@language":"en","@value":"Nakanuma Yuji"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Department of Physics, Toyama University"}]},{"@id":"https://cir.nii.ac.jp/crid/1410001204187528067","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197288"},{"@type":"NRID","@value":"9000002591816"},{"@type":"NRID","@value":"9000401891225"}],"foaf:name":[{"@language":"en","@value":"Fukuda Shuichi"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Department of Physics, Toyama University"}]},{"@id":"https://cir.nii.ac.jp/crid/1410001204187528066","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197290"},{"@type":"NRID","@value":"9000401891227"}],"foaf:name":[{"@language":"en","@value":"Sakurai Junji"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Department of Physics, Toyama University"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801206046464","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"20334708"},{"@type":"NRID","@value":"1000020334708"},{"@type":"ORCID","@value":"0000-0003-1087-6666"},{"@type":"NRID","@value":"9000107351839"},{"@type":"NRID","@value":"9000024992881"},{"@type":"NRID","@value":"9000241168592"},{"@type":"NRID","@value":"9000401797400"},{"@type":"NRID","@value":"9000401890840"},{"@type":"NRID","@value":"9000398817611"},{"@type":"NRID","@value":"9000415095749"},{"@type":"NRID","@value":"9000398958597"},{"@type":"NRID","@value":"9000017674213"},{"@type":"NRID","@value":"9000412201375"},{"@type":"NRID","@value":"9000415058704"},{"@type":"NRID","@value":"9000401973513"},{"@type":"NRID","@value":"9000401883078"},{"@type":"NRID","@value":"9000025117506"},{"@type":"NRID","@value":"9000244889700"},{"@type":"NRID","@value":"9000415060070"},{"@type":"NRID","@value":"9000258197291"},{"@type":"NRID","@value":"9000415096606"},{"@type":"NRID","@value":"9000241658931"},{"@type":"NRID","@value":"9000401972714"},{"@type":"NRID","@value":"9000241541152"},{"@type":"NRID","@value":"9000401910885"},{"@type":"NRID","@value":"9000010268739"},{"@type":"NRID","@value":"9000415112538"},{"@type":"NRID","@value":"9000242835024"},{"@type":"NRID","@value":"9000346926101"},{"@type":"NRID","@value":"9000018261316"},{"@type":"NRID","@value":"9000401888058"},{"@type":"NRID","@value":"9000258187795"},{"@type":"NRID","@value":"9000412104621"},{"@type":"NRID","@value":"9000401966058"},{"@type":"NRID","@value":"9000401875444"},{"@type":"NRID","@value":"9000415112593"},{"@type":"NRID","@value":"9000345326129"},{"@type":"NRID","@value":"9000415059768"},{"@type":"NRID","@value":"9000388463300"},{"@type":"NRID","@value":"9000401965615"},{"@type":"NRID","@value":"9000401975182"},{"@type":"NRID","@value":"9000401891228"},{"@type":"NRID","@value":"9000410867559"},{"@type":"NRID","@value":"9000415052822"},{"@type":"NRID","@value":"9000401998269"},{"@type":"NRID","@value":"9000258197167"},{"@type":"NRID","@value":"9000415112506"},{"@type":"NRID","@value":"9000415114092"},{"@type":"NRID","@value":"9000006346769"},{"@type":"NRID","@value":"9000244888940"},{"@type":"NRID","@value":"9000401912358"},{"@type":"NRID","@value":"9000409646753"},{"@type":"NRID","@value":"9000340441957"},{"@type":"NRID","@value":"9000415059422"},{"@type":"NRID","@value":"9000401976474"},{"@type":"NRID","@value":"9000401976298"},{"@type":"NRID","@value":"9000401890402"},{"@type":"NRID","@value":"9000415112562"},{"@type":"NRID","@value":"9000018457625"},{"@type":"NRID","@value":"9000356648524"},{"@type":"NRID","@value":"9000244886626"},{"@type":"NRID","@value":"9000401885701"},{"@type":"NRID","@value":"9000401902055"},{"@type":"NRID","@value":"9000401898995"},{"@type":"NRID","@value":"9000018887500"},{"@type":"NRID","@value":"9000410518770"},{"@type":"NRID","@value":"9000415058032"},{"@type":"NRID","@value":"9000410622269"},{"@type":"NRID","@value":"9000401886987"},{"@type":"NRID","@value":"9000415113013"},{"@type":"NRID","@value":"9000415096619"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0061044"}],"foaf:name":[{"@language":"en","@value":"Mitsuda Akihiro"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Department of Physics, Toyama University"}]},{"@id":"https://cir.nii.ac.jp/crid/1410001204187528070","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258197292"},{"@type":"NRID","@value":"9000401891229"}],"foaf:name":[{"@language":"en","@value":"Isikawa Yosikazu"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Department of Physics, Toyama University"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319015"},{"@type":"LISSN","@value":"00319015"},{"@type":"EISSN","@value":"13474073"},{"@type":"NDL_BIB_ID","@value":"000000118709"},{"@type":"ISSN","@value":"00319015"},{"@type":"NCID","@value":"AA00704814"}],"prism:publicationName":[{"@language":"en","@value":"Journal of the Physical Society of Japan"},{"@language":"ja","@value":"Ｊｏｕｒｎａｌ　ｏｆ　ｔｈｅ　Ｐｈｙｓｉｃａｌ　Ｓｏｃｉｅｔｙ　ｏｆ　Ｊａｐａｎ"},{"@language":"en","@value":"JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN"},{"@language":"en","@value":"JPSJ"},{"@language":"ja","@value":"ＪＰＳＪ"}],"dc:publisher":[{"@language":"en","@value":"THE PHYSICAL SOCIETY OF JAPAN"},{"@language":"ja","@value":"一般社団法人 日本物理学会"}],"prism:publicationDate":"2003","prism:volume":"72","prism:number":"12","prism:startingPage":"3189","prism:endingPage":"3196"},"reviewed":"false","url":[{"@id":"http://id.ndl.go.jp/bib/6789471"},{"@id":"https://ndlsearch.ndl.go.jp/books/R000000004-I6789471"},{"@id":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.72.3189"}],"availableAt":"2003","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=thermoelectric%20power","dc:title":"thermoelectric power"},{"@id":"https://cir.nii.ac.jp/all?q=specific%20heat","dc:title":"specific heat"},{"@id":"https://cir.nii.ac.jp/all?q=valence%20transition","dc:title":"valence transition"},{"@id":"https://cir.nii.ac.jp/all?q=Doniach%20diagram","dc:title":"Doniach diagram"},{"@id":"https://cir.nii.ac.jp/all?q=EuCu%3CSUB%3E2%3C/SUB%3E(Si%3CI%3E%3CSUB%3Ex%3C/SUB%3E%3C/I%3EGe%3CSUB%3E1%E2%88%92%3CI%3Ex%3C/I%3E%3C/SUB%3E)%3CSUB%3E2%3C/SUB%3E","dc:title":"EuCu<SUB>2</SUB>(Si<I><SUB>x</SUB></I>Ge<SUB>1−<I>x</I></SUB>)<SUB>2</SUB>"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360002221358500352","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Unique Pressure versus Temperature Phase Diagram for Antiferromagnets Eu<sub>2</sub>Ni<sub>3</sub>Ge<sub>5</sub>and EuRhSi<sub>3</sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360003446870705920","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Pressure-Induced Valence Transition in Antiferromagnet EuRh<sub>2</sub>Si<sub>2</sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285707213749248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Anomalous ferromagnetic ordering in EuCuP"}]},{"@id":"https://cir.nii.ac.jp/crid/1360568469886645632","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electronic states of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mi>EuCu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Ge</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mi>EuCu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Si</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>\n studied by soft x-ray photoemission spectroscopy"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095729243264","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy fermion state in CeCu6"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659921960576","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Kondo-like behavior near the magnetic instability in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi mathvariant=\"bold\">SmB</mml:mi><mml:mn mathvariant=\"bold\">6</mml:mn></mml:msub></mml:math>\n: Temperature and pressure dependences of the Sm valence"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593664806784","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electronic structure of the intermediate-valence compound \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mi>EuNi</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant=\"normal\">P</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>\n studied by soft x-ray photoemission spectroscopy"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995011693440","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@value":"The Kondo lattice and weak antiferromagnetism"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470086862848","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Charge Fluctuations in Europium in Metallic Eu<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">Cu</mml:mi></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\">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544418593532928","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Design of an XAFS beamline at the Photon Factory: possibilities of bent conical mirrors"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544421031972480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Critical evaluation of Eu valences from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"italic\">L</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant=\"normal\">III</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>-edge x-ray-absorption and Mössbauer spectroscopy of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">EuNi</mml:mi></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\">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi mathvariant=\"normal\">−</mml:mi><mml:mi mathvariant=\"italic\">x</mml:mi></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\">Ge</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant=\"italic\">x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825896017683968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Rare Earth Intermetallics: Thermopower of Cerium, Samarium, and Europium Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107368238991616","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Test for the cumulant approximation in the critical region"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369664852352","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Thermodynamic and transport properties of CeCu6"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269103250304","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Thermoelectric power of EuNi2(Si1−xGex)2"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269380922240","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Pressure effect on the valence transition of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">EuNi</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">Ge</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mi>−</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">Si</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><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>"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269742058880","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A new and unique Eu-based mixed valence system: EuPd<sub>2</sub>Si<sub>2</sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204188009344","@type":"Article","relationType":["isReferencedBy","isCitedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Correlation of Initial Slope of Thermoelectric Power and Electronic Specific-Heat Constant for Solid Solutions Based on Ce and Eu Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282679162853760","@type":"Article","relationType":["references","cites"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Valence Transition between Eu2+ State and Eu3+ State in EuxY1-xPd2Si2 and EuxLa1-xPd2Si2"},{"@value":"Valence Transition between Eu〔2+〕 State and Eu〔3+〕 State in EuxY1-xPd2Si2 and EuxLa1-xPd2Si2"},{"@value":"Valence Transition between Eu<sup>2+</sup>State and Eu<sup>3+</sup>State in Eu<sub><i>x</i></sub>Y<sub>1-<i>x</i></sub>Pd<sub>2</sub>Si<sub>2</sub>and Eu<sub><i>x</i></sub>La<sub>1-<i>x</i></sub>Pd<sub>2</sub>Si<sub>2</sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1520291854880252672","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electronic States in EuCu₂(Ge₁₋xSi[x])₂ Based on the Doniach Phase Diagram"}]},{"@id":"https://cir.nii.ac.jp/crid/1520573329808857088","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Effects of Magnetic Field and Pressure on the Valence-Fluctuating Antiferromagnetic Compound EuPt₂Si₂"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854805919538816","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Spin Glass Behavior in EuCu₂Si₂ Single Crystal Grown by the Flux Method"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854806045144960","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Magnetization Process in EuCo₂P₂ and EuT₂Ge₂ (T: transition metal) : Comparison of Experiment and Theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854806265206784","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy Fermion Emerging from the Singular Fermi Liquid in Underscreened Kondo Model for Eu Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1521699230597279872","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quantum Criticality of Valence Transition for the Unique Electronic State of Antiferromagnetic Compound EuCu₂Ge₂"}]},{"@id":"https://cir.nii.ac.jp/crid/1521980705428331520","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Unique Electronic States of Eu-based Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1522825130397281792","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Theory of Magnetic Ordering and Valence Fluctuation in Nearly Trivalent Eu Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1523388080809915648","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Valence Fluctuation, Spin-Orbit Coupling, and Magnetic-Nonmagnetic Crossover in Eu Compounds"}]},{"@id":"https://cir.nii.ac.jp/crid/1570009749993439488","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1570291224970150016","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1570572699746843520","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1570572699932622208","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1571135649700096128","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1571698599839466368","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1571980074816175616","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1571980074830415232","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1572261549792887680","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1572824499602947840","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573105974537239296","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573105974579657472","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573387449699729792","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573668924634424576","@type":"Article","relationType":["cites"]},{"@id":"https://cir.nii.ac.jp/crid/1573950401498468608","@type":"Article","relationType":["cites"]}],"dataSourceIdentifier":[{"@type":"JALC","@value":"oai:japanlinkcenter.org:0023493174"},{"@type":"NDL_SEARCH","@value":"oai:ndlsearch.ndl.go.jp:R000000004-I6789471"},{"@type":"CROSSREF","@value":"10.1143/jpsj.72.3189"},{"@type":"CIA","@value":"130004538358"},{"@type":"CIA","@value":"110001954365"},{"@type":"CIA","@value":"210000104602"},{"@type":"OPENAIRE","@value":"doi_dedup___::01584b80e5a7c8b83d113d2b528a64e0"},{"@type":"CROSSREF","@value":"10.1143/jpsj.81.023709_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.1143/jpsj.74.1926_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.034705_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.053703_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.88.113705_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.102001_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.86.034708_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.1103/physrevb.100.035111_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.90.123702_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.1103/physrevb.97.161116_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.87.064706_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.87.074709_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.1103/physrevb.104.165124_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.90.034709_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.124711_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"},{"@type":"CROSSREF","@value":"10.1016/j.jallcom.2019.02.213_references_DOI_3Jkv9QWYW81r54cPdg47PLRuWXW"}]}