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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:10.1103/PhysRevB.99.054419</dc:identifier><dc:language>eng</dc:language><dc:creator>Marcano, N.</dc:creator><dc:creator>Algarabel, P.A.</dc:creator><dc:creator>Barquín, L.F.</dc:creator><dc:creator>Araujo, J.P.</dc:creator><dc:creator>Pereira, A.M.</dc:creator><dc:creator>Belo, J.H.</dc:creator><dc:creator>Magén, C.</dc:creator><dc:creator>Morellón, L.</dc:creator><dc:creator>Ibarra, M.R.</dc:creator><dc:title>Cluster-glass dynamics of the Griffiths phase in Tb5-xLaxSi2Ge2</dc:title><dc:identifier>ART-2019-111231</dc:identifier><dc:description>The static magnetization and dynamic susceptibility responses of the cluster system within a Griffiths phase of the magnetocaloric compound Tb5-xLaxSi2Ge2 (x=0.075) have been investigated. A novel cluster-glass state within the Griffiths phase is formed at a characteristic freezing temperature where short-range ferromagnetic correlations set in the paramagnetic regime. Ferromagneticlike correlations are built up at around 155 K, which suddenly become frozen at a lower temperature ~140K, thus in analogy with a reentrant spin glass behavior. The ac susceptibility near the freezing temperature follows a critical slowing down process characterized by t0=10-13s and dynamic exponents z¿~6 and ß~0.4, similar to well-known spin glass systems. The nonlinear ac susceptibility analysis shows clearly the existence of a transition associated to the reentrant behavior. The origin of the intermediate cluster-glass phase inside the Griffiths phase is proposed to be the result of a combination of short-ranged RKKY intralayer positive exchange interactions between rare-earth Tb3+ ions and antiferromagnetic exchange between adjacent interlayers involving Si and Ge atoms in connection to the Tb3+ atoms.</dc:description><dc:date>2019</dc:date><dc:source>http://zaguan.unizar.es/record/78858</dc:source><dc:doi>10.1103/PhysRevB.99.054419</dc:doi><dc:identifier>http://zaguan.unizar.es/record/78858</dc:identifier><dc:identifier>oai:zaguan.unizar.es:78858</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E26</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MCIU/MAT2017-83631-C3-R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/MAT2017-82970-C2-2-R</dc:relation><dc:identifier.citation>PHYSICAL REVIEW B 99, 5 (2019), 054419 [10 pp]</dc:identifier.citation><dc:rights>by-nc</dc:rights><dc:rights>http://creativecommons.org/licenses/by-nc/3.0/es/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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