2013
DOI: 10.1103/physrevd.88.056014
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Functional renormalization group study of the two-flavor linear sigma model in the presence of the axial anomaly

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Cited by 51 publications
(45 citation statements)
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“…In the presence of the axial anomaly in terms of the 't Hooft determinant this transition is expected to be of second order in the O(4) universality class [21]. If, however, the U (1) A -symmetry were restored at the chiral transition, a first order transition or a second order transition in the universality class of U (2) L × U (2) R /U (2) A could take place [22][23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…In the presence of the axial anomaly in terms of the 't Hooft determinant this transition is expected to be of second order in the O(4) universality class [21]. If, however, the U (1) A -symmetry were restored at the chiral transition, a first order transition or a second order transition in the universality class of U (2) L × U (2) R /U (2) A could take place [22][23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…The breaking of the U(1) A symmetry at finite T , and its role at the chiral transition, has been much investigated [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34]. Monte Carlo (MC) simulations of lattice QCD [17][18][19][20][21][22][23][24][25] find a substantial suppression of the U(1) A anomaly effects at large T , as predicted by the DIG model.…”
Section: Introductionmentioning
confidence: 99%
“…O(4) model [9]. However, if the anomaly is already sufficiently restored at T c , the transition is either first or second order with a different symmetry breaking pattern [67,68]. For recent lattice studies of the U A (1) anomaly see, e.g.…”
Section: Universal Critical Behavior and The Qcd Phase Diagrammentioning
confidence: 99%