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dc.contributor.authorTomiya, A.en
dc.contributor.authorCossu, G.en
dc.contributor.authorAoki, S.en
dc.contributor.authorFukaya, H.en
dc.contributor.authorHashimoto, S.en
dc.contributor.authorKaneko, T.en
dc.contributor.authorNoaki, J.en
dc.contributor.authorJLQCD Collaborationen
dc.contributor.alternative青木, 愼也ja
dc.date.accessioned2020-04-13T12:37:33Z-
dc.date.available2020-04-13T12:37:33Z-
dc.date.issued2017-08-01-
dc.identifier.issn2470-0010-
dc.identifier.urihttp://hdl.handle.net/2433/250234-
dc.description.abstractWe study the axial U(1) symmetry at a finite temperature in two-flavor lattice QCD. Employing the Mobius domain-wall fermions, we generate gauge configurations slightly above the critical temperature Tc with different lattice sizes L = 2-4 fm. Our action allows frequent topology tunneling while keeping good chiral symmetry close enough to that of overlap fermions. This allows us to recover full chiral symmetry by an overlap/domain-wall reweighting. Above the phase transition, a strong suppression of the low-lying modes is observed in both overlap and domain-wall Dirac spectra. We, however, find a sizable violation of the Ginsparg-Wilson relation in the Mobius domain-wall Dirac eigenmodes, which dominates the signals of the axial U(1) symmetry breaking near the chiral limit. We also find that the use of the overlap fermion only in the valence sector is dangerous since it suffers from the artifacts due to partial quenching. Reweighting the Mobius domain-wall fermion determinant to that of the overlap fermion, we observe the axial U(1) breaking to vanish in the chiral limit, which is stable against the changes of the lattice volume and lattice spacing.en
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherAmerican Physical Society (APS)en
dc.rights© 2017 American Physical Societyen
dc.titleEvidence of effective axial U(1) symmetry restoration at high temperature QCDen
dc.typejournal article-
dc.type.niitypeJournal Article-
dc.identifier.jtitlePhysical Review Den
dc.identifier.volume96-
dc.identifier.issue3-
dc.relation.doi10.1103/PhysRevD.96.034509-
dc.textversionpublisher-
dc.identifier.artnum034509-
dc.addressKey Laboratory of Quark & Lepton Physics (MOE) and Institute of Particle Physics, Central China Normal Universityen
dc.addressSchool of Physics and Astronomy, The University of Edinburghen
dc.addressCenter for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto Universityen
dc.addressDepartment of Physics, Graduate School of Science, Osaka Universityen
dc.addressHigh Energy Accelerator Research Organization (KEK)・School of High Energy Accelerator Science, The Graduate University for Advanced Studies (Sokendai)en
dc.addressHigh Energy Accelerator Research Organization (KEK)・School of High Energy Accelerator Science, The Graduate University for Advanced Studies (Sokendai)en
dc.addressHigh Energy Accelerator Research Organization (KEK)en
dcterms.accessRightsopen access-
datacite.awardNumberJP25800147-
datacite.awardNumberJP26247043-
datacite.awardNumberJP26400259-
datacite.awardNumberJP15K05065-
datacite.awardNumberJP16H03978-
jpcoar.funderName日本学術振興会ja
jpcoar.funderName日本学術振興会ja
jpcoar.funderName日本学術振興会ja
jpcoar.funderName日本学術振興会ja
jpcoar.funderName日本学術振興会ja
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
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