Pseudoscalar Screening Mass at Finite Temperature and Magnetic Field from Lattice QCD with Physical Quark Masses

TL;DR

This study uses lattice QCD simulations to analyze how the screening mass of neutral pseudoscalar mesons varies with temperature and magnetic field, providing insights into QCD matter under extreme conditions.

Contribution

First lattice QCD results on pseudoscalar screening masses at finite temperature and magnetic field with physical quark masses.

Findings

Screening masses increase with temperature and magnetic field.

Magnetic field influences mesonic properties near the QCD transition.

Results help understand QCD phase transitions in extreme environments.

Abstract

Understanding the screening mass of pseudoscalar mesons at finite temperature and magnetic field is crucial for comprehending the behavior of strongly interacting matter under extreme conditions, such as those found in the early universe or inside neutron stars. Additionally, in heavy ion collisions, strong magnetic fields are generated, which could significantly influence the properties of the quark-gluon plasma. The study of these screening masses provides insight into the modifications of mesonic properties in such environments, which is essential for the theoretical understanding of Quantum Chromodynamics (QCD) phase transitions and the properties of the quark-gluon plasma. Here, we present continuum estimated lattice QCD results on the screening mass of neutral pseudoscalar mesons at finite temperatures and nonzero magnetic fields. The simulations used (2+1)-flavor lattice QCD simulations using physical quark masses employing the HISQ/tree action. The continuum estimation was carried out using lattices having temporal extents $N_\tau$ = 8, 12, and 16, all having aspect ratio $N_\sigma/N_\tau$ = 4. The investigated temperature ranges from 145 MeV to 166 MeV, while the magnetic field strength varies from 0 to 1 GeV$^2$. We discuss the dependence of the screening masses of various neutral pseudoscalar mesons on temperature, magnetic field strength, and quark mass.