<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-04-17T16:06:43Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/174988" metadataPrefix="qdc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/174988</identifier><datestamp>2025-11-21T05:49:47Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478823</setSpec><setSpec>col_2072_478904</setSpec><setSpec>col_2072_478917</setSpec></header><metadata><qdc:qualifieddc xmlns:qdc="http://dspace.org/qualifieddc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://purl.org/dc/elements/1.1/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dc.xsd http://purl.org/dc/terms/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dcterms.xsd http://dspace.org/qualifieddc/ http://www.ukoln.ac.uk/metadata/dcmi/xmlschema/qualifieddc.xsd">
   <dc:title>Phases of unitary matrix models and lattice QCD2</dc:title>
   <dc:creator>Russo, J. G. (Jorge Guillermo)</dc:creator>
   <dc:subject>Matèria condensada</dc:subject>
   <dc:subject>Teoria de camps (Física)</dc:subject>
   <dc:subject>Condensed matter</dc:subject>
   <dc:subject>Field theory (Physics)</dc:subject>
   <dcterms:abstract>We investigate the different large N phases of a generalized Gross-Witten-Wadia (GWW) U(N) matrix model. The deformation mimics the one-loop determinant of fermion matter with a particular coupling to gauge fields. In one version of the model, the GWW phase transition is smoothed out and it becomes a crossover. In another version, the phase transition occurs along a critical line in the two-dimensional parameter space spanned by the 't Hooft coupling λ and the Veneziano parameter τ. We compute the expectation value of Wilson loops in both phases, showing that the transition is third order. A calculation of the β function shows the existence of an IR stable fixed point.</dcterms:abstract>
   <dcterms:issued>2021-03-12T10:21:58Z</dcterms:issued>
   <dcterms:issued>2021-03-12T10:21:58Z</dcterms:issued>
   <dcterms:issued>2020-11-23</dcterms:issued>
   <dcterms:issued>2021-03-12T10:21:58Z</dcterms:issued>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevD.102.105019</dc:relation>
   <dc:relation>Physical Review D, 2020, vol. 102, num. 10, p. 105019</dc:relation>
   <dc:relation>https://doi.org/10.1103/PhysRevD.102.105019</dc:relation>
   <dc:rights>cc-by (c) Russo, J.G., 2020</dc:rights>
   <dc:rights>http://creativecommons.org/licenses/by/3.0/es/</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:publisher>American Physical Society</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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