Abstract

We discuss density corrections of the chiral condensate up to a NLO order us- ing the chiral Ward identity and an in-medium chiral perturbation theory. The in-medium chiral condensate is calculated by a correlation function of the axial current and pseu- doscalar density in the nuclear matter as a consequence of the chiral Ward identity. The correlation function is evaluated using the chiral perturbation theory with the hadronic quantities of pion-nucleon dynamics. We assume that the in-vacuum interaction vertices are known, which means that the in-vacuum loop corrections are renormalized to the tree chiral couplings by taking the values of the couplings in chiral Lagrangian as the physical values. We focus on density order in the physical quantities in our perturbative calcula- tion. This study shows that the medium effects to the chiral condensate beyond the linear density come from density corrections to theN sigma term. It implies that calculating the density dependence of the chiral condensate in nuclear matter is essentially equivalent to describe nuclear matter in chiral effective theory.

Highlights

  • Chiral symmetry breaking SU(N f )L ⊗ SU(N f )R → SU(N f )V is an important phenomenon, which characterizes low-energy Quantum ChromoDynamics(QCD) and Hadron physics, and the nonvanishing chiral condensate qq as an order parameter of χSSB generates hadron masses.Recently, partial restoration of chiral symmetry in the nuclear medium has gained considerable attention

  • The in-medium chiral condensate is calculated by a correlation function of the axial current and pseudoscalar density in the nuclear matter as a consequence of the chiral Ward identity

  • This study shows that the medium effects to the chiral condensate beyond the linear density come from density corrections to the πN sigma term

Read more

Summary

Introduction

Chiral symmetry breaking (χSSB) SU(N f )L ⊗ SU(N f )R → SU(N f )V is an important phenomenon, which characterizes low-energy Quantum ChromoDynamics(QCD) and Hadron physics, and the nonvanishing chiral condensate qq as an order parameter of χSSB generates hadron masses. Partial restoration of chiral symmetry in the nuclear medium has gained considerable attention. Qq ∗, qq 0 are the in-medium and in-vacuum chiral condensates, respectively, and ρ0 is the normal nuclear density This estimation suggests that the chiral symmetry breaking is partially restored. It is important to evaluate the in-medium condensate quantitatively

Chiral Ward identity
In-medium chiral perturbation theory
Density dependence of chiral condensate
Summary
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call