Quark–Gluon plasma driven by the strong force is subject to the conservativeness of the
baryon number, net electric charge, strangeness, etc. However, the fluctuations around their …

We investigate the effect of a background magnetic field when applied to a nonextensive
QCD medium in a\(2+ 1\) flavour Nambu—Jona-Lasinio model. The effect of a constant as …

To describe the chiral magnetic effect, the chiral chemical potential $\mu_5 $ is introduced to
imitate the impact of topological charge changing transitions in the quark-gluon plasma …

In the QCD-like effective model, the Polyakov linear-sigma model, the isospin sigma field (σ¯
3= f K±− f K 0) and the third generator of the matrix of the explicit symmetry breaking [h 3 …

In present work, we extend Lüscher formula-like formalism to few-body system in a uniform
magnetic field with Dirichlet boundary conditions. As a signature of non-trivial topological …

The influence of non-extensive Tsallis statistics on the hadron phase structure has been
investigated using the Polyakov-quark-meson (PQM) model. The analysis examines the non …

We calculate the gluon self-energy using quark energy projectors in a general quark-gluon
plasma. By separating the quark field into positive-and a negative-energy modes, the quark …

The recent research work of two-flavor quarks with magnetised Polyakov–Nambu–Jona–
Lasinio (mPNJL) model has been upgraded with the inclusion of a finite chemical potential …

The mass spectrum of different meson particles is generated using an effective Lagrangian
of the extended linear-sigma model (eLSM) for scalar and pseudoscalar meson fields and …

Mapping out phase diagrams of quantum systems using classical simulations can be
challenging or intractable due to the computational resources required to simulate even …