We calculate the screening masses of pseudoscalar mesons in a hot and strongly magnetized medium within the framework of the SU(3) Nambu-Jona–Lasinio model, using a magnetic field-independent regularization scheme. Inverse magnetic catalysis (IMC) is implemented through the use of a magnetic field-dependent coupling G(B), fitted to reproduce lattice quantum chromodynamics (QCD) results for the pseudocritical chiral transition temperature TcB. For the external homogeneous magnetic field considered, neutral screening masses separate in two types: perpendicular and parallel to the direction of the field, while for charged mesons only parallel energies can be defined for each Landau level. We obtain mscr,⊥>mscr,||, as expected from causality. Thermally, all screening energies are almost constant until some critical temperature, whose behavior is correlated with TcB. They rapidly increase around this value, keeping a steady enhancement afterward due to thermal excitation. Magnetically, neutral parallel masses are enhanced (suppressed) at high temperatures when considering G(B) (G). Perpendicular ones display a nonmonotonic magnetic behavior for G (due to increasing TcB) when T≲500 MeV, but become magnetically enhanced when T≳500 MeV. For G(B) they always increase with B. Charged parallel energies are always magnetically enhanced, for both couplings. In the high-temperature limit, we show that both neutral and charged screening energies converge to 2πT. At B=0 the model overestimates the remaining quark interaction in this regime. At B≠0 we find that, when IMC is accounted for, the interaction is suppressed as B increases, a fact that appears to be at odds with currently available lattice QCD results.
Published by the American Physical Society
2024