Abstract

We construct the most general low-energy effective lagrangian including local parity violating terms parametrized by an axial chemical potential or chiral imbalance μ5, up to mathcal{O}left({p}^4right) order in the chiral expansion for two light flavours. For that purpose, we work within the Chiral Perturbation Theory framework where only pseudo-NGB fields are included, following the external source method. The mathcal{O}left({p}^2right) lagrangian is only modified by constant terms, while the mathcal{O}left({p}^4right) one includes new terms proportional to {mu}_5^2 and new low-energy constants (LEC), which are renormalized and related to particular observables. In particular, we analyze the corrections to the pion dispersion relation and observables related to the vacuum energy density, namely the light quark condensate, the chiral and topological susceptibilities and the chiral charge density, providing numerical determinations of the new LEC when possible. In particular, we explore the dependence of the chiral restoration temperature Tc with μ5. An increasing Tc(μ5) is consistent with our fits to lattice data of the ChPT-based expressions. Although lattice uncertainties are still large and translate into the new LEC determination, a consistent physical description of those observables emerges from our present work, providing a theoretically robust model-independent framework for further study of physical systems where parity-breaking effects may be relevant, such as heavy-ion collisions.

Highlights

  • A convenient way to parametrize such a P -breaking source or chiral imbalance is by means of a constant axial chemical potential μ5 to be added to the QCD action over a given finite space-time region

  • We construct the most general low-energy effective lagrangian including local parity violating terms parametrized by an axial chemical potential or chiral imbalance μ5, up to O(p4) order in the chiral expansion for two light flavours

  • We analyze the corrections to the pion dispersion relation and observables related to the vacuum energy density, namely the light quark condensate, the chiral and topological susceptibilities and the chiral charge density, providing numerical determinations of the new lowenergy constants (LEC) when possible

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Summary

Construction of the effective lagrangian

Let us follow the same procedure as before, to O(p4) The lagrangian to this order will consist of the usual SU(2) terms in [7, 8, 31] with the covariant derivative dμ in (2.3), plus new terms constructed out of the Q operators and the operator tr(U †dμU ), as commented above. As discussed in appendix B, SU(2) operator identities allow to reduce the number of independent terms After these considerations, the lagrangian without explicit Q fields is the usual one in [31], where the μ5 corrections are those containing the covariant derivative dμ in (2.3), namely, L04.

Pion dispersion relation
The vacuum energy density
The topological susceptibility
Pressure and speed of sound
Conclusions
Terms with no Q fields
Findings
C Useful integrals in dimensional regularization
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