The hadronization process for quarks combining into two mesons, qq→ MM′ at
temperature T is described within the SU (3) Nambu–Jona-Lasinio model with finite current …

In this article, there are 18 sections discussing various current topics in the field of relativistic
heavy-ion collisions and related phenomena, which will serve as a snapshot of the current …

We solve a nonlocal generalisation of the NJL model in the Hartree approximation. This
model has a separable interaction, as suggested by instanton models of the QCD vacuum …

We consider a non-local version of the NJL model, based on a separable quark-quark
interaction. The interaction is extended to include terms that bind vector and axial-vector …

A nonlocal chiral quark model is consistently extended beyond mean field using a strict 1/N
c expansion scheme. The parameters of the nonlocal model are refitted so that the physical …

In the framework of the Nambu–Jona-Lasinio model beyond mean field approximation, the
effects of pion fluctuations on (inverse) magnetic catalysis and magnetic susceptibility are …

We have calculated the temperature dependence of shear η and bulk ζ viscosities of quark
matter due to quark-meson fluctuations. The quark thermal width originating from quantum …

We study the equation of state of QCD using an improved version of the three-flavor
Polyakov–Nambu–Jona-Lasinio model beyond the mean-field approximation. It …

The s-wave π-π scattering lengths a1 (T) at finite temperature T and isospin I= 0, 2 are
calculated within the SU (2) Nambu-Jona-Lasinio model. a2 (T) displays a singularity at the …

We study the meson contribution to the equation of state of the 2-flavor Polyakov-loop
Nambu–Jona-Lasinio model, including the full momentum dependence of the meson …