Rotation lowers critical temperatures for chiral and deconfinement transitions in the Polyakov linear sigma model under causality constraints, with mechanical properties computed in the homogeneous limit.
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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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Linear sigma model with quarks and Polyakov loop in rotation: phase diagrams, Tolman-Ehrenfest law and mechanical properties
Rotation lowers critical temperatures for chiral and deconfinement transitions in the Polyakov linear sigma model under causality constraints, with mechanical properties computed in the homogeneous limit.
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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.