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Phases and condensates in zero-temperature QCD at finite μ I and μ S
I discuss pion and kaon condensation and the the properties of the phases of QCD at finite isospin chemical potential μ I and strangeness chemical potential μ S at zero temperature using three-flavor chiral perturbation theory. Electromagnetic effects are included in the calculation of the phase dia...
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Main Author: | |
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Format: | Conference Proceeding |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | I discuss pion and kaon condensation and the the properties of the phases of QCD at finite isospin chemical potential
μ
I
and strangeness chemical potential
μ
S
at zero temperature using three-flavor chiral perturbation theory. Electromagnetic effects are included in the calculation of the phase diagram, which implies that the charged meson condensed phases become superconducting phases of QCD with a massive photon via the Higgs mechanism. Without electromagnetic effects, we show results for the light quark condensate and the pion condensate as functions of
μ
I
at next-to-leading (NLO) order in the lowenergy expansion. The results are compared with recent lattice simulations and by including the NLO corrections, one obtains very good agreement. |
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ISSN: | 2100-014X 2101-6275 2100-014X |
DOI: | 10.1051/epjconf/202227407003 |