{"@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/1390282679154897152.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1143/jpsj.60.760"}},{"identifier":{"@type":"BIBCODE","@value":"1991JPSJ...60..760T"}},{"identifier":{"@type":"NDL_BIB_ID","@value":"3714553"}},{"identifier":{"@type":"URI","@value":"http://id.ndl.go.jp/bib/3714553"}},{"identifier":{"@type":"URI","@value":"https://ndlsearch.ndl.go.jp/books/R000000004-I3714553"}},{"identifier":{"@type":"URI","@value":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.60.760"}},{"identifier":{"@type":"NAID","@value":"110001977175"}},{"identifier":{"@type":"NAID","@value":"130003740912"}},{"identifier":{"@type":"NAID","@value":"210000096557"}}],"dc:title":[{"@language":"en","@value":"Magnetization Curve and Correlation Function of Haldane-Gap Antiferromagnet in Strong Magnetic Field"},{"@language":"ja-Kana","@value":"Magnetization Curve and Correlation Fun"}],"dc:language":"en","description":[{"type":"abstract","notation":[{"@language":"en","@value":"The shape of the magnetization curve of the <I>S</I>=1 Heisenberg antiferromagnet at zero temperature is discussed. It is found that the magnetization behaves as \\sqrt<I>h</I>−<I>h<SUB>c</SUB></I> at the beginning of magnetization as a function of external field <I>h</I>. The transverse correlation function ⟨<I>S</I><SUB>0</SUB><I><SUP>x</SUP>S<SUB>n</SUB><SUP>x</SUP></I>⟩=⟨<I>S</I><SUB>0</SUB><I><SUP>y</SUP>S<SUB>n</SUB><SUP>y</SUP></I>⟩ of this system decays algebraically at zero temperature when it is partially magnetized by the field to the <I>z</I>-direction (⟨<I>S</I><SUB>0</SUB><I><SUP>x</SUP>S<SUB>n</SUB><SUP>x</SUP></I>⟩\\simeq(−1)<I><SUP>n</SUP>n</I><SUP>−η</SUP>). The exponent η is 0.3∼0.5. This exponent can be calculated by the Luttinger liquid assumption and diagonalization results of finite chains. This is in contrast to the exponential decay of this chain in zero field."}],"abstractLicenseFlag":"disallow"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1410282679154897153","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000254139153"},{"@type":"NRID","@value":"9000401865825"}],"foaf:name":[{"@language":"en","@value":"Takahashi Minoru"}],"jpcoar:affiliationName":[{"@language":"en","@value":"Institute for Solid State Physics, University of 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