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        <identifier>oai:hiroshima.repo.nii.ac.jp:02007214</identifier>
        <datestamp>2025-02-21T09:27:45Z</datestamp>
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        <jpcoar:jpcoar xmlns:datacite="https://schema.datacite.org/meta/kernel-4/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcndl="http://ndl.go.jp/dcndl/terms/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:jpcoar="https://github.com/JPCOAR/schema/blob/master/2.0/" xmlns:oaire="http://namespace.openaire.eu/schema/oaire/" xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:rioxxterms="http://www.rioxx.net/schema/v2.0/rioxxterms/" xmlns:xs="http://www.w3.org/2001/XMLSchema" xmlns="https://github.com/JPCOAR/schema/blob/master/2.0/" xsi:schemaLocation="https://github.com/JPCOAR/schema/blob/master/2.0/jpcoar_scm.xsd">
          <dc:title xml:lang="en">Magnetic diagnostics using the third-harmonic magnetic response for a molecule-based magnet networked by a single chiral ligand</dc:title>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Mito, Masaki</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Mito</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">Masaki</jpcoar:givenName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Iriguchi, K.</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Iriguchi</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">K.</jpcoar:givenName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Deguchi, Hiroyuki</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Deguchi</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">Hiroyuki</jpcoar:givenName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Kishine, Jun-Ichiro</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Kishine</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">Jun-Ichiro</jpcoar:givenName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Yoshida, Yusuke</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Yoshida</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">Yusuke</jpcoar:givenName>
          </jpcoar:creator>
          <jpcoar:creator>
            <jpcoar:creatorName xml:lang="en">Inoue, Katsuya</jpcoar:creatorName>
            <jpcoar:familyName xml:lang="en">Inoue</jpcoar:familyName>
            <jpcoar:givenName xml:lang="en">Katsuya</jpcoar:givenName>
          </jpcoar:creator>
          <dcterms:accessRights rdf:resource="http://purl.org/coar/access_right/c_abf2">open access</dcterms:accessRights>
          <dc:rights>(c) 2012 American Institute of Physics</dc:rights>
          <jpcoar:subject subjectScheme="NDC">430</jpcoar:subject>
          <datacite:description xml:lang="en">We investigated complex magnetic domain formation on a chiral molecule-based magnet, [Cr(CN)6][Mn(R)-pnH(H2O)](H2O) (termed as R-GN), whose two-dimensional molecular network was constructed with the help of a single-handed chiral ligand ((R)-pn). There, the first- and third-harmonic magnetic responses (M1ω and M3ω) against the ac magnetic field were observed, and magnetic hysteresis in ac field of a few Oe was discussed in terms of Rayleigh loop. The diagnostics of this magnetic hysteresis clarified the complex process of magnetic domain formation against a change in temperature. For R-GN, it was reported that a giant M3ω (termed #4 in this paper) appeared just above the so-called “magnetic ordering temperature (TC)." In the present study, three M3ω responses (#1-3) were newly observed on the lower-temperature side of #4, and the ac field dependencies for all of #1-#4 were investigated. #1 also accompanied the giant M3ω, which suggests that a significant degree of magnetic fluctuation surviving below TC. This glassy behavior below TC is an attractive new phenomenon in molecule-based magnets with a single-handed chiral ligand. #2 and #3 exhibited magnetic ordering and the formation of a small magnetic domain, respectively. The M3ω responses of #1-3 were suppressed with increasing the amplitude of ac field, and the corresponding magnetic hysteresis was a normal Rayleigh loop accompanying the out-of-phase of the M1ω response. The M3ω response of #4 without the out-of-phase of M1ω was, however, enhanced with increasing the amplitude of ac field, and #4 represented a large magnetic hysteresis in the paramagnetic region, intrinsically different from those of #1-#3.</datacite:description>
          <dc:publisher>American Institute of Physics</dc:publisher>
          <datacite:date dateType="Issued">2012</datacite:date>
          <dc:language>eng</dc:language>
          <dc:type rdf:resource="http://purl.org/coar/resource_type/c_6501">journal article</dc:type>
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          <jpcoar:identifier identifierType="URI">https://hiroshima.repo.nii.ac.jp/records/2007214</jpcoar:identifier>
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            <jpcoar:relatedIdentifier identifierType="DOI">10.1063/1.4721806</jpcoar:relatedIdentifier>
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            <jpcoar:relatedIdentifier identifierType="DOI">http://dx.doi.org/10.1063/1.4721806</jpcoar:relatedIdentifier>
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          <jpcoar:sourceIdentifier identifierType="ISSN">0021-8979</jpcoar:sourceIdentifier>
          <jpcoar:sourceIdentifier identifierType="NCID">AA00693547</jpcoar:sourceIdentifier>
          <jpcoar:sourceTitle>Journal of Applied Physics</jpcoar:sourceTitle>
          <jpcoar:sourceTitle>Journal of Applied Physics</jpcoar:sourceTitle>
          <jpcoar:volume>111</jpcoar:volume>
          <jpcoar:issue>10</jpcoar:issue>
          <jpcoar:pageStart>103914</jpcoar:pageStart>
          <jpcoar:pageStart>103914</jpcoar:pageStart>
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