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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1039/c9dt04816b</dc:identifier><dc:language>eng</dc:language><dc:creator>Rubín, Javier</dc:creator><dc:creator>Badía-Romano, Laura</dc:creator><dc:creator>Luis, Fernando</dc:creator><dc:creator>Mereacre, Valeriu</dc:creator><dc:creator>Prodius, Denis</dc:creator><dc:creator>Arauzo, Ana</dc:creator><dc:creator>Bartolomé, Fernando</dc:creator><dc:creator>Bartolomé, Juan</dc:creator><dc:title>Magnetic chains of Fe3 clusters in the {Fe3YO2} butterfly molecular compound</dc:title><dc:identifier>ART-2020-117220</dc:identifier><dc:description>The "butterfly" molecule [Fe3Y(µ3-O)2(CCl3COO)8(H2O)(THF)3] (in brief {Fe3YO2}) includes three Fe3+ ions which build a robust Fe3 cluster with a strong intracluster antiferromagnetic exchange and a total spin S = 5/2. It represents the starting magnetic system to study further interactions with magnetic rare earths when Y is replaced with lanthanides. We present heat capacity and equilibrium susceptibility measurements below 2 K, which show that each cluster has a sizeable magnetic anisotropy pointing to the existence of intercluster interactions. However, no phase transition to a long-range magnetically ordered phase is observed down to 20 mK. The intercluster interaction is analysed in the framework of the one-dimensional Blume-Capel model with an antiferromagnetic chain interaction constant J/kB = -40(2) mK between Fe3 cluster spins, and a uniaxial anisotropy with parameter D/kB = -0.56(3) K. This is associated to single chains of Fe3 clusters oriented along the shortest intercluster distances displayed by the crystal structure of {Fe3YO2}. Ac susceptibility measurements reveal that the magnetic relaxation is dominated by a quantum tunnelling process below 0.2 K, and by thermally activated processes above this temperature. The experimental activation energy of this single chain magnet, Ea/kB = 3.4(6) K, can be accounted for by the combination of contributions arising from single-molecule magnetic anisotropy and spin-spin correlations along the chains.</dc:description><dc:date>2020</dc:date><dc:source>http://zaguan.unizar.es/record/149132</dc:source><dc:doi>10.1039/c9dt04816b</dc:doi><dc:identifier>http://zaguan.unizar.es/record/149132</dc:identifier><dc:identifier>oai:zaguan.unizar.es:149132</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E09-17R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E12-R17</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCINN/MAT2017-83468-R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCINN/PCI2018-093116</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/RTI2018-096075-B-C21</dc:relation><dc:relation>info:eu-repo/grantAgreement/EUR/MOLSPIN-COST/CA15128</dc:relation><dc:identifier.citation>Dalton Transactions 49, 9 (2020), 2979-2988</dc:identifier.citation><dc:rights>All rights reserved</dc:rights><dc:rights>http://www.europeana.eu/rights/rr-f/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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