Abstract

In this work the neutral meson properties have been investigated in the presence of thermo-magnetic background using two-flavor Nambu--Jona-Lasinio model. Mass, spectral function and dispersion relations are obtained in the scalar ($\sigma$) and pseudo-scalar ($\pi^0$) channels as well as in the vector ($\rho^0$) and axial vector ($a^0_1$) channels. The general Lorentz structures for the vector and axial-vector meson polarization functions have been considered in detail. The ultra-violet divergences appearing in this work have been regularized using a mixed regularization technique where the gamma functions arising in dimensional regularization are replaced with incomplete gamma functions as usually done in the proper time regularization procedure. The meson spectral functions obtained in the presence of a magnetic field possess nontrivial oscillatory structure. Similar to the scalar and pseudo-scalar channel, the spectral functions for each of the modes of $\rho^0$ are observed to overlap with the corresponding modes of its chiral partner $a_1^0$ mesons in the chiral symmetry restored phase. We observe discontinuities in the masses of all the mesonic excitations for a non-zero external magnetic field.

Highlights

  • Based on a considerable amount of research regarding the generation of magnetic fields in noncentral heavy ion collision (HIC), there exists a growing consensus that an extremely strong transient magnetic field of the order of ∼1018 G or larger can be produced at the RHIC and the LHC [1,2,3,4,5,6,7,8]

  • The ultraviolet divergences appearing in this work have been regularized using a mixed regularization technique where the gamma functions arising in dimensional regularization are replaced with incomplete gamma functions as is usually done in the proper time regularization procedure

  • Similar to the scalar and pseudoscalar channel, the spectral functions for each of the modes of ρ0 are observed to overlap with the corresponding modes of its chiral partner a01 mesons in the chiral symmetry restored phase

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Summary

Introduction

Based on a considerable amount of research regarding the generation of magnetic fields in noncentral heavy ion collision (HIC), there exists a growing consensus that an extremely strong transient magnetic field of the order of ∼1018 G or larger can be produced at the RHIC and the LHC [1,2,3,4,5,6,7,8]. At lower temperatures, the usual field theoretic approach of studying quantum chromodynamics (QCD) is not feasible due to the confining nature of strong interaction that severely restricts the applicability of perturbative analysis. In this scenario, an alternative to the nonperturbative lattice QCD approach is provided by the QCD inspired effective models. An alternative to the nonperturbative lattice QCD approach is provided by the QCD inspired effective models The modification of such effective descriptions in the presence of an external magnetic field has gained significant research interests in recent times [26]. One such model is the Nambu–Jona-Lasinio model [27,28,29,30,31,32] which has been widely used in the studies of chiral symmetry breaking as well as meson properties in the presence of thermo-magnetic background [33,34,35,36]

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