{"@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/1390282679158427136.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1143/jpsj.65.1178"}},{"identifier":{"@type":"BIBCODE","@value":"1996JPSJ...65.1178I"}},{"identifier":{"@type":"URI","@value":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.65.1178"}},{"identifier":{"@type":"NAID","@value":"130004535621"}},{"identifier":{"@type":"NAID","@value":"210000099273"}}],"dc:title":[{"@language":"en","@value":"Magnetic Susceptibility of Quasi-One-Dimensional Compound .ALPHA.'-NaV2O5. Possible Spin-Peierls Compound with High Critical Temperature of 34K."},{"@value":"Magnetic Susceptibility of Quasi-One-Dimensional Compound<i>α'-<b><i>N</i><i>a</i><i>V</i><sub>2</sub><i>O</i><sub>5</sub></b></i>–Possible Spin-Peierls Compound with High Critical Temperature of 34 K–"}],"dc:language":"en","description":[{"type":"abstract","notation":[{"@language":"en","@value":"Stoichiometric powder samples of α '-NaV<SUB>2</SUB>O<SUB>5</SUB> were synthesized and the magnetic susceptibility was measured in the temperature range from 2, K to 700, K. The magnetic susceptibility has a good fit to the equation for an S=1/2 antiferromagnetic Heisenberg linear chain with J/k<SUB>B</SUB>=280, K and g=2 above 34, K. Below 34, K the magnetic susceptibility rapidly decreases with decreasing temperature to a constant value of 1.49× 10<SUP>-4</SUP>, emu/V<SUP>4+</SUP>-mol which is reasonable for spin-singlet V<SUP>4+</SUP>--V<SUP>4+</SUP> pairs. This rapid reduction of the spin susceptibility below 34, K suggests the existence of a spin-Peierls transition. α '-NaV<SUB>2</SUB>O<SUB>5</SUB> is a possible spin-Peierls compound with the highest critical temperature yet observed."}],"abstractLicenseFlag":"disallow"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1410001204179781248","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000401871738"},{"@type":"NRID","@value":"9000283263150"},{"@type":"NRID","@value":"9000258188340"},{"@type":"NRID","@value":"9000258191388"},{"@type":"NRID","@value":"9000401888366"},{"@type":"NRID","@value":"9000258189002"},{"@type":"NRID","@value":"9000401888004"},{"@type":"NRID","@value":"9000401897577"},{"@type":"NRID","@value":"9000258194571"},{"@type":"NRID","@value":"9000258196411"},{"@type":"NRID","@value":"9000258191028"},{"@type":"NRID","@value":"9000401873999"},{"@type":"NRID","@value":"9000401884174"},{"@type":"NRID","@value":"9000401877699"},{"@type":"NRID","@value":"9000258194646"},{"@type":"NRID","@value":"9000401874704"},{"@type":"NRID","@value":"9000401875171"},{"@type":"NRID","@value":"9000401878255"},{"@type":"NRID","@value":"9000401882229"},{"@type":"NRID","@value":"9000258194212"},{"@type":"NRID","@value":"9000401886017"},{"@type":"NRID","@value":"9000401880795"},{"@type":"NRID","@value":"9000401880790"},{"@type":"NRID","@value":"9000000819245"},{"@type":"NRID","@value":"9000045463161"},{"@type":"NRID","@value":"9000401889287"},{"@type":"NRID","@value":"9000401878837"},{"@type":"NRID","@value":"9000401877148"},{"@type":"NRID","@value":"9000401877565"},{"@type":"NRID","@value":"9000258189060"},{"@type":"NRID","@value":"9000258190598"},{"@type":"NRID","@value":"9000258195462"},{"@type":"NRID","@value":"9000258195022"},{"@type":"NRID","@value":"9000401878147"},{"@type":"NRID","@value":"9000258191101"},{"@type":"NRID","@value":"9000401883853"},{"@type":"NRID","@value":"9000401883677"},{"@type":"NRID","@value":"9000401880199"},{"@type":"NRID","@value":"9000401887286"},{"@type":"NRID","@value":"9000401885058"},{"@type":"NRID","@value":"9000258189448"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0003318"}],"foaf:name":[{"@language":"en","@value":"Isobe Masahiko"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Institute for Solid State Physics, The University of Tokyo, Roppongi 7–22–1, Minato–ku, Tokyo 106"}]},{"@id":"https://cir.nii.ac.jp/crid/1410282679158427137","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000258188341"},{"@type":"NRID","@value":"9000401874000"}],"foaf:name":[{"@language":"en","@value":"Ueda Yutaka"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Institute for Solid State Physics, The University of Tokyo, Roppongi 7–22–1, Minato–ku, Tokyo 106"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319015"},{"@type":"LISSN","@value":"00319015"},{"@type":"EISSN","@value":"13474073"}],"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":"1996","prism:volume":"65","prism:number":"5","prism:startingPage":"1178","prism:endingPage":"1181"},"reviewed":"false","url":[{"@id":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.65.1178"}],"availableAt":"1996","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=%CE%B1'-%20NaV%3CSUB%3E2%3C/SUB%3EO%3CSUB%3E5%3C/SUB%3E","dc:title":"α'- NaV<SUB>2</SUB>O<SUB>5</SUB>"},{"@id":"https://cir.nii.ac.jp/all?q=magnetic%20susceptibility","dc:title":"magnetic susceptibility"},{"@id":"https://cir.nii.ac.jp/all?q=S%3D1/2%20antiferromagnetic%20Heisenberg%20linear%20chain","dc:title":"S=1/2 antiferromagnetic Heisenberg linear chain"},{"@id":"https://cir.nii.ac.jp/all?q=spin-Peierls%20transition","dc:title":"spin-Peierls transition"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050291768349742464","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Achieving Superconductivity with Higher Tc in Lightweight Al-Ti-Mg Alloys: Prediction using Machine Learning and Synthesis via High-Pressure Torsion Process"},{"@value":"Achieving superconductivity with higher <i>T</i>c in lightweight Al–Ti–Mg alloys: Prediction using machine learning and synthesis via high-pressure torsion process"}]},{"@id":"https://cir.nii.ac.jp/crid/1050867133851969280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"51V-NMR study of charge order induced by cation order in δ-Ag2/3V2O5"},{"@value":"<sup>51</sup>V-NMR study of charge order induced by cation order in 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mathvariant=\"normal\">O</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Comprising Spin-½ Quasi-1D Two-Leg Ladders"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262945484857344","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Affinement de la structure cristalline du bronze NaV2O5α'"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233271012227968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Observation of the spin-Peierls transition in linear<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=\"normal\">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>(spin-1/2) chains in an inorganic compound<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">CuGeO</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204179831296","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Raman, Infrared and Optical Spectra of the Spin-Peierls Compound NaV2O5."},{"@language":"ja-Kana","@value":"Raman Infrared and Optical Spectra of t"},{"@value":"Raman, Infrared and Optical Spectra of the Spin-Peierls Compound NaV<sub><b>2</b></sub>O<sub><b>5</b></sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204179965952","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Electron Diffraction Study of the Phase Transformation of .ALPHA.'-NaV2O5."},{"@value":"Electron Diffraction Study of the Phase Transformation of<i>α'</i>-NaV<sub><b>2</b></sub>O<sub><b>5</b></sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204180520960","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Optical Conductivity of the Trellis-Lattice t-J Model: Charge Fluctuations in NaV2O5."},{"@language":"ja-Kana","@value":"Optical Conductivity of the Trellis-Lat"},{"@value":"Optical Conductivity of the Trellis-Lattice <i> <i>t</i></i>-<i> <i>J</i></i> Model:    Charge Fluctuations in NaV<sub><b> 2</b></sub>O<sub><b> 5</b></sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204180540416","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Direct Observation of the Spin Gap in NaV2O5 by Submillimeter Wave ESR."},{"@language":"ja-Kana","@value":"Direct Observation of the Spin Gap in N"},{"@value":"Direct Observation of the Spin Gap in NaV<sub><b> 2</b></sub>O<sub><b> 5</b></sub>    by Submillimeter Wave ESR"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204180587904","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Spin Dynamics of the One-Dimensional J-J Model and Spin-Peierls Transition in CuGeO3."},{"@value":"Spin Dynamics of the One-Dimensional J-J′ Model and Spin-Peierls Transition in CuGeO3"},{"@language":"ja-Kana","@value":"Spin Dynamics of the One-Dimensional J-"},{"@value":"Spin Dynamics of the One-Dimensional<i><i>J</i></i>-<i><i>J</i></i>' Model and Spin-Peierls Transition in CuGeO<sub><b>3</b></sub>"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204181333248","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"On the Magnetic Properties of Systems with Low Dimensional Linkage of VO5 Pyramids."},{"@language":"ja-Kana","@value":"On the Magnetic Properties of Systems w"},{"@value":"On the Magnetic Properties of Systems with Low Dimensional Linkage of 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