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<identifier>oai:icatplus.esrf.fr:inv/2376081184</identifier>
<datestamp>2026-05-11T06:00:54.844Z</datestamp>
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<identifier identifierType="DOI">10.15151/ESRF-ES-2376081184</identifier>
<creators>
<creator>
<creatorName nameType="Personal">Maksim RYZHKOV</creatorName>
<givenName>Maksim</givenName>
<familyName>Ryzhkov</familyName>
</creator>
<creator>
<creatorName nameType="Personal">Xin LIU</creatorName>
<givenName>Xin</givenName>
<familyName>Liu</familyName>
<nameIdentifier nameIdentifierScheme="ORCID">0000-0002-2631-277X</nameIdentifier>
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<creator>
<creatorName nameType="Personal">Fabrice WILHELM</creatorName>
<givenName>Fabrice</givenName>
<familyName>Wilhelm</familyName>
<nameIdentifier nameIdentifierScheme="ORCID">0000-0002-4425-3662</nameIdentifier>
</creator>
<creator>
<creatorName nameType="Personal">Xin LIU</creatorName>
<givenName>Xin</givenName>
<familyName>Liu</familyName>
<nameIdentifier nameIdentifierScheme="ORCID">0000-0002-2631-277X</nameIdentifier>
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<creator>
<creatorName nameType="Personal">Maksim RYZHKOV</creatorName>
<givenName>Maksim</givenName>
<familyName>Ryzhkov</familyName>
</creator>
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<titles>
<title>Full-angle spin rotation in multiferroic GdMn2O5 (continuatuion)</title>
</titles>
<publisher>Example Institute</publisher>
<publicationYear>2029</publicationYear>
<resourceType resourceTypeGeneral="Collection">Data from large facility measurement</resourceType>
<dates>
<date dateType="Collected">2026-05-05T06:00:00Z/2026-05-11T06:00:00Z</date>
<date dateType="Accepted">2026-05-11T06:00:00Z</date>
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<rights rightsIdentifier="CC-BY-4.0" rightsURI="https://creativecommons.org/licenses/by/4.0">CC-BY-4.0</rights>
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<description descriptionType="Abstract">Recently, an unusual sequence of four topological states has been observed in multiferroic GdMn2O5 [1]. In these experiments, in ramping the external magnetic field up and down through the magnetic phase transition, the electric polarization of the sample passes through a cycle of four states, schematically represented as 1→2→3→4→1. In these experiments, the clockwise or counterclockwise sequence of states is protected by the geometry of the experiment, making them equivalent to a topological charge. A theoretical explanation of the observed effects suggests that half of the spins rotate by 360° with 90° in each step. The goal of this proposal is to observe the full-angle spin rotation with the field-induced XMLD.</description>
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