QCD phase diagram in a magnetized medium from the chiral symmetry perspective: The linear sigma model with quarks and the Nambu--Jona-Lasinio model effective descriptions

TL;DR

This paper reviews how effective models like the linear sigma model with quarks and the Nambu--Jona-Lasinio model describe the QCD phase diagram under magnetic fields, emphasizing plasma screening effects and phenomena like inverse magnetic catalysis.

Contribution

It highlights the importance of plasma screening effects in effective models for understanding magnetic field influences on the QCD phase diagram, including the inverse magnetic catalysis phenomenon.

Findings

Screening effects are crucial for modeling phase transitions.

Inverse magnetic catalysis can occur without magnetic field-dependent couplings.

The critical end point's location depends on interaction types and magnetic field dependence.

Abstract

We review the main features of the QCD phase diagram description, at finite temperature, baryon density and in the presence of a magnetic field, from the point of view of effective models, whose main ingredient is chiral symmetry. We concentrate our attention on two of these models: The linear sigma model with quarks and the Nambu--Jona-Lasinio model. We show that a main ingredient to understand the characteristics of the phase transitions is the inclusion of plasma screening effects that capture the physics of collective, long-wave modes, and thus describe a prime property of plasmas near transition lines, namely, long distance correlations. Inclusion of plasma screening makes possible to understand the inverse magnetic catalysis phenomenon even without the need to consider magnetic field-dependent coupling constants. Screening is also responsible for the emergence of a critical end point in the phase diagram even for small magnetic field strengths. Although versatile, the NJL model is also a more limited approach since, being a non-renormalizable model, a clear separation between pure vacuum and medium effects is not always possible. The model cannot describe inverse magnetic catalysis unless a magnetic field dependent coupling is included. The location of the critical end point strongly depends on the choice of the type of interaction and on the magnetic field dependence of the corresponding coupling. Overall, both models provide sensible tools to explore the properties of magnetized, strongly interacting matter. However, a cross talk among them as well as a consistent physical approach to determine the model parameters is much needed.