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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/PhysRevD.97.014507</dc:identifier><dc:language>eng</dc:language><dc:creator>Azcoiti, V.</dc:creator><dc:creator>Follana, E.</dc:creator><dc:creator>Royo-Amondarain, E.</dc:creator><dc:creator>Di Carlo, G.</dc:creator><dc:creator>Vaquero Avilés-Casco, A.</dc:creator><dc:title>Massive Schwinger model at finite ¿</dc:title><dc:identifier>ART-2018-104659</dc:identifier><dc:description>Using the approach developed by V. Azcoiti et al. [Phys. Lett. B 563, 117 (2003)PYLBAJ0370-269310.1016/S0370-2693(03)00601-4], we are able to reconstruct the behavior of the massive one-flavor Schwinger model with a ¿ term and a quantized topological charge. We calculate the full dependence of the order parameter with ¿. Our results at ¿=p are compatible with Coleman''s conjecture on the phase diagram of this model.</dc:description><dc:date>2018</dc:date><dc:source>http://zaguan.unizar.es/record/69669</dc:source><dc:doi>10.1103/PhysRevD.97.014507</dc:doi><dc:identifier>http://zaguan.unizar.es/record/69669</dc:identifier><dc:identifier>oai:zaguan.unizar.es:69669</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E24-2</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/FPA2015-65745-P</dc:relation><dc:identifier.citation>Physical Review D 97, 1 (2018), 014507 [8 pp]</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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