2015
DOI: 10.1103/physrevc.92.015214
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Chiral mirror-baryon-meson model and nuclear matter beyond mean-field approximation

Abstract: We consider a chiral baryon-meson model for nucleons and their parity partners in mirror assignment interacting with pions, sigma and omega mesons to describe the liquid-gas transition of nuclear matter together with chiral symmetry restoration in the high density phase. Within the mean-field approximation the model is known to provide a phenomenologically successful description of the nuclear-matter transition. Here, we go beyond this approximation and include mesonic fluctuations by means of the functional r… Show more

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Cited by 50 publications
(42 citation statements)
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“…We see again that at T = 0, fluctuations show up at µ B = m N , but by reaching µ c , the relative changes are less than 10%; thus, the SB violation remains small. Note that no first order chiral transition is observed beyond µ c , similarly as found in [22] (the other jump in the order parameters, related to the nuclear liquid-gas transition, is in turn missing due to the absence of the dynamics of a neutral vector meson [24,28]). …”
Section: Resultsmentioning
confidence: 68%
“…We see again that at T = 0, fluctuations show up at µ B = m N , but by reaching µ c , the relative changes are less than 10%; thus, the SB violation remains small. Note that no first order chiral transition is observed beyond µ c , similarly as found in [22] (the other jump in the order parameters, related to the nuclear liquid-gas transition, is in turn missing due to the absence of the dynamics of a neutral vector meson [24,28]). …”
Section: Resultsmentioning
confidence: 68%
“…Very recently liquid-gas and chiral phase transition are studied in a parity doublet model with a six-point scalar interaction in which mesonic fluctuations are included by means of the functional renormalization group [15]. In this work we study isospin asymmetric dense matter in the framework of the parity doublet model (mirror assignment) [16,17].…”
Section: Introductionmentioning
confidence: 99%
“…Phenomenologically viable spectral functions also require the inclusion of the feedback of the vector mesons themselves as well as baryonic degrees of freedom, both of which have been neglected here. Especially given the fact that our approach allows for the computation of spectral functions also at arbitrarily large chemical potential calls for an extension to include the dynamics of baryons and nuclear-matter effects in a chiral effective theory that is capable of describing both, the liquid-gas transition of nuclear matter and the chiral transition in a unified framework [55]. Several of these issues have been addressed already within the FRG, showing that this method is flexible enough to tackle these ambitious tasks in the future.…”
Section: Discussionmentioning
confidence: 99%