Renormalization group invariant mean-field model for QCD at finite isospin density

Fuente: arXiv
Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Brandt, Bastian B., Chelnokov, Volodymyr, Endrodi, Gergely, Marko, Gergely, Scheid, Daniel, von Smekal, Lorenz
Format: Preprint
Veröffentlicht: 2025
Schlagworte:
Online-Zugang:
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
_version_ 1866911139749691392
author Brandt, Bastian B.
Chelnokov, Volodymyr
Endrodi, Gergely
Marko, Gergely
Scheid, Daniel
von Smekal, Lorenz
author_facet Brandt, Bastian B.
Chelnokov, Volodymyr
Endrodi, Gergely
Marko, Gergely
Scheid, Daniel
von Smekal, Lorenz
contents QCD at nonzero isospin chemical potentials has phenomenological relevance for a series of physical systems and provides an ideal testground for the modeling of dense strongly interacting matter. The two-flavor quark-meson model is known to effectively describe the condensation of charged pions in QCD that occurs in this setting. In this paper, we derive a renormalization-group invariant mean-field formulation of the model and demonstrate that the resulting phase diagram and equation of state are in quantitative agreement with data from lattice QCD simulations at small and intermediate isospin chemical potentials. In particular, the speed of sound from the model shows an excess over the conformal bound as previously seen in lattice computations in agreement with chiral perturbation theory. We then consider the speed of sound in the limit of large isospin chemical potentials and see that it approaches the conformal limit from above, in qualitative agreement with recent lattice results and in quantitative agreement with perturbation theory in the presence of a BCS gap. Finally, we consider the phase diagram in the approach to the chiral limit. We find that within the model the chiral phase transition connects to the pion condensation phase boundary in the chiral limit and we discuss the implications for the properties of the chiral transition point.
format Preprint
id arxiv_https___arxiv_org_abs_2502_04025
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Renormalization group invariant mean-field model for QCD at finite isospin density
Brandt, Bastian B.
Chelnokov, Volodymyr
Endrodi, Gergely
Marko, Gergely
Scheid, Daniel
von Smekal, Lorenz
High Energy Physics - Phenomenology
High Energy Physics - Lattice
Nuclear Theory
QCD at nonzero isospin chemical potentials has phenomenological relevance for a series of physical systems and provides an ideal testground for the modeling of dense strongly interacting matter. The two-flavor quark-meson model is known to effectively describe the condensation of charged pions in QCD that occurs in this setting. In this paper, we derive a renormalization-group invariant mean-field formulation of the model and demonstrate that the resulting phase diagram and equation of state are in quantitative agreement with data from lattice QCD simulations at small and intermediate isospin chemical potentials. In particular, the speed of sound from the model shows an excess over the conformal bound as previously seen in lattice computations in agreement with chiral perturbation theory. We then consider the speed of sound in the limit of large isospin chemical potentials and see that it approaches the conformal limit from above, in qualitative agreement with recent lattice results and in quantitative agreement with perturbation theory in the presence of a BCS gap. Finally, we consider the phase diagram in the approach to the chiral limit. We find that within the model the chiral phase transition connects to the pion condensation phase boundary in the chiral limit and we discuss the implications for the properties of the chiral transition point.
title Renormalization group invariant mean-field model for QCD at finite isospin density
topic High Energy Physics - Phenomenology
High Energy Physics - Lattice
Nuclear Theory
url https://arxiv.org/abs/2502.04025