2017
DOI: 10.1007/jhep04(2017)036
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Symmetry restoration at high-temperature in two-color and two-flavor lattice gauge theories

Abstract: We consider the SU(2) gauge theory with N f = 2 flavors of Dirac fundamental fermions. We study the high-temperature behavior of the spectra of mesons, discretizing the theory on anisotropic lattices, and measuring the two-point correlation functions in the temporal direction as well as screening masses in various channels. We identify the (pseudo-)critical temperature as the temperature at which the susceptibility associated with the Polyakov loop has a maximum. At high temperature both the spin-1 and spin-0 … Show more

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Cited by 29 publications
(41 citation statements)
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“…These results are consistent with previous analysis of screening masses by the same group [40]. Another lattice analysis based on meson screening masses pointing towards Uð1Þ A restoration taking place above T c is [41], for two flavors and two colors. On the other hand, the lattice results in [42][43][44] are consistent with Uð1Þ A restoration taking place at the chiral transition or very close above it.…”
Section: Introductionsupporting
confidence: 92%
“…These results are consistent with previous analysis of screening masses by the same group [40]. Another lattice analysis based on meson screening masses pointing towards Uð1Þ A restoration taking place above T c is [41], for two flavors and two colors. On the other hand, the lattice results in [42][43][44] are consistent with Uð1Þ A restoration taking place at the chiral transition or very close above it.…”
Section: Introductionsupporting
confidence: 92%
“…As in Ref. [50], it is convenient to label the broken generators with A = 1 , · · · , 5, and the unbroken ones with A = 6 , · · · , 15. We hence add to the Lagrangian density the following source term:…”
Section: F1 Su (4)/sp(4) Composite Operatorsmentioning
confidence: 99%
“…We adopt the same basis as in Ref. [50], and within these conventions we find the following: 13 and O µ V,14 would be the unbroken generators in the SU (2) L × SU (2) R /SU (2) V coset, corresponding to the ρ mesons in QCD, in which case O µ V,15 would be associated with baryon number and would source the ω/φ in QCD.…”
Section: F1 Su (4)/sp(4) Composite Operatorsmentioning
confidence: 99%
“…Four of the PNGBs of the resulting EFT are interpreted as the Higgs doublet, hence providing an elegant symmetry argument for the lightness of the associated particles. Particular attention has been devoted to models based on the SU (4)/Sp(4) coset [8,[26][27][28][29][30][31][32][33][34][35][36][37], as EFT arguments suggest that the resulting phenomenology is both realistic and rich enough to motivate a more systematic study of the underlying dynamics. This coset emerges naturally in gauge theories with pseudo-real representations, such as Sp(2N ) gauge theories with two massless Dirac fermions in the fundamental representation of the gauge group.…”
Section: The Sp(2n ) Research Programmementioning
confidence: 99%