Chiral symmetry restoration at nonzero temperature in the SU(3){sub r}xSU(3){sub l} linear sigma model
We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the SU(3){sub r}xSU(3){sub l} linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are sy...
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Veröffentlicht in: | Physical review. D, Particles and fields Particles and fields, 2000-10, Vol.62 (8) |
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creator | Lenaghan, Jonathan T. Rischke, Dirk H. Schaffner-Bielich, Ju''rgen |
description | We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the SU(3){sub r}xSU(3){sub l} linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the U(1){sub A} anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing. |
doi_str_mv | 10.1103/PhysRevD.62.085008 |
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Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the U(1){sub A} anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing.</description><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PhysRevD.62.085008</identifier><language>eng</language><publisher>United States: The American Physical Society</publisher><subject>CHIRAL SYMMETRY ; CONDENSATES ; ENANTIOMORPHS ; HARTREE-FOCK METHOD ; MESONS ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; PSEUDOSCALAR MESONS ; QUARKS ; SCALARS ; SIGMA MODEL</subject><ispartof>Physical review. 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D, Particles and fields</title><description>We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the SU(3){sub r}xSU(3){sub l} linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the U(1){sub A} anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing.</description><subject>CHIRAL SYMMETRY</subject><subject>CONDENSATES</subject><subject>ENANTIOMORPHS</subject><subject>HARTREE-FOCK METHOD</subject><subject>MESONS</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>PSEUDOSCALAR MESONS</subject><subject>QUARKS</subject><subject>SCALARS</subject><subject>SIGMA MODEL</subject><issn>0556-2821</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><recordid>eNpFjE1LAzEYhIMoWKt_wFPAix625mOTTY5S6wcUFLXnkk3fdSO7iSSpuEr_uwsKzmWYh5lB6JSSGaWEXz62Q3qCj-uZZDOiBCFqD00oUbooNVX7aEKEkAVTjB6io5TeyCgm-QQ189ZF0-E09D3kOOAIKYdosgsem4x98F8QA87Qv8OItxGw8zi3gJ9X5_ziO21rHHef_6Hb4c55MBEn99ob3IcNdMfooDFdgpM_n6LVzeJlflcsH27v51fLIlDKc2EpY6qpdWkbSbW2wpBNxaSqQNXG2NLUlpWaN8RoIbWttK5hrNWVJHScMT5FZ7-_IWW3TtZlsK0N3oPN65IwIqjg_AcloFsS</recordid><startdate>20001015</startdate><enddate>20001015</enddate><creator>Lenaghan, Jonathan T.</creator><creator>Rischke, Dirk H.</creator><creator>Schaffner-Bielich, Ju''rgen</creator><general>The American Physical Society</general><scope>OTOTI</scope></search><sort><creationdate>20001015</creationdate><title>Chiral symmetry restoration at nonzero temperature in the SU(3){sub r}xSU(3){sub l} linear sigma model</title><author>Lenaghan, Jonathan T. ; Rischke, Dirk H. ; Schaffner-Bielich, Ju''rgen</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o113t-c1228fb94cf6199c5a0d72687e8baac4abc2493f0a9569c799be99cb7601fb923</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2000</creationdate><topic>CHIRAL SYMMETRY</topic><topic>CONDENSATES</topic><topic>ENANTIOMORPHS</topic><topic>HARTREE-FOCK METHOD</topic><topic>MESONS</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>PSEUDOSCALAR MESONS</topic><topic>QUARKS</topic><topic>SCALARS</topic><topic>SIGMA MODEL</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lenaghan, Jonathan T.</creatorcontrib><creatorcontrib>Rischke, Dirk H.</creatorcontrib><creatorcontrib>Schaffner-Bielich, Ju''rgen</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physical review. D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lenaghan, Jonathan T.</au><au>Rischke, Dirk H.</au><au>Schaffner-Bielich, Ju''rgen</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Chiral symmetry restoration at nonzero temperature in the SU(3){sub r}xSU(3){sub l} linear sigma model</atitle><jtitle>Physical review. D, Particles and fields</jtitle><date>2000-10-15</date><risdate>2000</risdate><volume>62</volume><issue>8</issue><issn>0556-2821</issn><eissn>1089-4918</eissn><abstract>We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the SU(3){sub r}xSU(3){sub l} linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the U(1){sub A} anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing.</abstract><cop>United States</cop><pub>The American Physical Society</pub><doi>10.1103/PhysRevD.62.085008</doi></addata></record> |
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subjects | CHIRAL SYMMETRY CONDENSATES ENANTIOMORPHS HARTREE-FOCK METHOD MESONS PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PSEUDOSCALAR MESONS QUARKS SCALARS SIGMA MODEL |
title | Chiral symmetry restoration at nonzero temperature in the SU(3){sub r}xSU(3){sub l} linear sigma model |
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