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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:10.1073/pnas.1203295109</dc:identifier><dc:language>eng</dc:language><dc:creator>Alvarez Baños, R.</dc:creator><dc:creator>Cruz, A.</dc:creator><dc:creator>Fernandez, L.A.</dc:creator><dc:creator>Gil-Narvion, J.M.</dc:creator><dc:creator>Gordillo-Guerrero, A.</dc:creator><dc:creator>Guidetti, M.</dc:creator><dc:creator>Iñiguez, D.</dc:creator><dc:creator>Maiorano, A.</dc:creator><dc:creator>Marinari, E.</dc:creator><dc:creator>Martin-Mayor, V.</dc:creator><dc:creator>Monforte-Garcia, J.</dc:creator><dc:creator>Muñoz-Sudupe, A.</dc:creator><dc:creator>Navarro, D.</dc:creator><dc:creator>Parisi, G.</dc:creator><dc:creator>Perez-Gaviro, S.</dc:creator><dc:creator>Ruiz-Lorenzo, J.J.</dc:creator><dc:creator>Schifano, S.F.</dc:creator><dc:creator>Seoane, B.</dc:creator><dc:creator>Tarancon, A.</dc:creator><dc:creator>Tellez, P.</dc:creator><dc:creator>Tripiccione, R.</dc:creator><dc:creator>Yllanes, D.</dc:creator><dc:title>Thermodynamic glass transition in a spin glass without time-reversal symmetry</dc:title><dc:identifier>ART-2012-82188</dc:identifier><dc:description>Spin glasses are a longstanding model for the sluggish dynamics that appear at the glass transition. However, spin glasses differ from structural glasses in a crucial feature: they enjoy a time reversal symmetry. This symmetry can be broken by applying an external magnetic field, but embarrassingly little is known about the critical behavior of a spin glass in a field. In this context, the space dimension is crucial. Simulations are easier to interpret in a large number of dimensions, but one must work below the upper critical dimension (i.e., in d &lt; 6) in order for results to have relevance for experiments. Here we show conclusive evidence for the presence of a phase transition in a four-dimensional spin glass in a field. Two ingredients were crucial for this achievement: massive numerical simulations were carried out on the Janus special-purpose computer, and a new and powerful finite-size scaling method.</dc:description><dc:date>2012</dc:date><dc:source>http://zaguan.unizar.es/record/152100</dc:source><dc:doi>10.1073/pnas.1203295109</dc:doi><dc:identifier>http://zaguan.unizar.es/record/152100</dc:identifier><dc:identifier>oai:zaguan.unizar.es:152100</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/FIS2009-12648-C03-02</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/FIS2010-16587</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/TEC2010-19207</dc:relation><dc:identifier.citation>Proceedings of the National Academy of Sciences of the United States of America 109, 17 (2012), 6452-6456</dc:identifier.citation><dc:rights>by-nc-nd</dc:rights><dc:rights>https://creativecommons.org/licenses/by-nc-nd/4.0/deed.es</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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