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dc.contributor.authorAdhikari, Prabal
dc.contributor.authorStrumke, Inga
dc.date.accessioned2024-03-11T08:51:30Z
dc.date.available2024-03-11T08:51:30Z
dc.date.created2023-11-27T11:16:27Z
dc.date.issued2023
dc.identifier.citationNuclear Physics B. 2023, 997 .en_US
dc.identifier.issn0550-3213
dc.identifier.urihttps://hdl.handle.net/11250/3121701
dc.description.abstractWe study three-flavor QCD in a uniform magnetic field using chiral perturbation theory (χPT). We construct the vacuum free energy density, quark condensate shifts induced by the magnetic field and the renormalized magnetization to O(p6) in the chiral expansion. We find that the calculation of the free energy is greatly simplified by cancellations among two-loop diagrams involving charged mesons. In comparing our results with recent -flavor lattice QCD data, we find that the light quark condensate shift at O(p6) is in better agreement than the shift at O(p4). We also find that the renormalized magnetization, due to its small-ness, possesses large uncertainties at due O(p6)to the uncertainties in the low-energy constants.en_US
dc.language.isoengen_US
dc.publisherElsevieren_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleVacuum free energy, quark condensate shifts and magnetization in three-flavor chiral perturbation theory to O(𝑝6) in a uniform magnetic fielden_US
dc.title.alternativeVacuum free energy, quark condensate shifts and magnetization in three-flavor chiral perturbation theory to O(p<sup>6</sup>) in a uniform magnetic fielden_US
dc.typePeer revieweden_US
dc.typeJournal articleen_US
dc.description.versionpublishedVersionen_US
dc.source.pagenumber0en_US
dc.source.volume997en_US
dc.source.journalNuclear Physics Ben_US
dc.identifier.doi10.1016/j.nuclphysb.2023.116389
dc.identifier.cristin2202796
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2


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