In the NJL model, rho meson masses for different charge and spin states increase or decrease with magnetic field at zero temperature, decrease with temperature at fixed B, approach constituent quark masses at high T, and exhibit degeneracies under combined finite B and T.
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Non-extensive NJL calculations show that the critical temperature Tc decreases with the Tsallis parameter q and that chiral chemical potential can switch the magnetic field effect from catalysis to inverse catalysis.
In the PNJL model, intermediate magnetic fields allow two or more first-order phase transitions in the light quark sector and produce entropy oscillations with rising baryon density.
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$\rho$ mesons in finite magnetic field and finite temperature
In the NJL model, rho meson masses for different charge and spin states increase or decrease with magnetic field at zero temperature, decrease with temperature at fixed B, approach constituent quark masses at high T, and exhibit degeneracies under combined finite B and T.
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Non-extensive NJL model study of QCD phase structure with chiral imbalance and strong magnetic fields
Non-extensive NJL calculations show that the critical temperature Tc decreases with the Tsallis parameter q and that chiral chemical potential can switch the magnetic field effect from catalysis to inverse catalysis.
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Deformed QCD phase structure and entropy oscillation in the presence of a magnetic background
In the PNJL model, intermediate magnetic fields allow two or more first-order phase transitions in the light quark sector and produce entropy oscillations with rising baryon density.