1996
DOI: 10.1103/physrevd.53.5142
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Effective action for the chiral quark-meson model

Abstract: The scale dependence of an effective average action for mesons and quarks is described by a nonperturbative flow equation. The running couplings lead to spontaneous chiral symmetry breaking. We argue that for strong Yukawa coupling between quarks and mesons the low momentum physics is essentially determined by infrared fixed points. This allows us to establish relations between various parameters related to the meson potential. The results for f π and ψψ are not very sensitive to the poorly known details of th… Show more

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Cited by 198 publications
(372 citation statements)
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“…An important property will be the observation that certain low energy properties are effectively independent of the details of the model even away from the phase transition. This behavior is caused by a strong attraction of the renormalization group flow to approximate partial infrared fixed points [167,28]. Within this approach at high density we find [212] a chiral symmetry restoring first order transition.…”
Section: Introductionmentioning
confidence: 85%
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“…An important property will be the observation that certain low energy properties are effectively independent of the details of the model even away from the phase transition. This behavior is caused by a strong attraction of the renormalization group flow to approximate partial infrared fixed points [167,28]. Within this approach at high density we find [212] a chiral symmetry restoring first order transition.…”
Section: Introductionmentioning
confidence: 85%
“…It is convenient to introduce two-parameter functions l d n 1 ,n 2 (w 1 , w 2 ; η) [167]. For n 1 = n 2 = 1 their relation to the functions l d n (w; η) can be expressed as…”
Section: Scaling Form Of the Flow Equationsmentioning
confidence: 99%
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“…This situation arises during the study of the phase diagram of QCD at non-zero temperature T and baryonic chemical potential µ [1,23,24,25]. An effective theory that captures many of the features of QCD is the quark-meson model [22]. It employs mesons and quarks as physical degrees of freedom.…”
Section: The Renormalization-group Flowmentioning
confidence: 99%
“…The full QCD dynamics cannot be described by an effective Lagrangian involving only mesonic fields. More complicated effective descriptions, such as the linear quark-meson model, have been used for the discussion of the phase diagram for low chemical potential [22,23,24]. In ref.…”
Section: Introductionmentioning
confidence: 99%