“…This coefficient was computed in hadronic kinetic theory [27], partonic transport models [39,40], off-shell transport and dynamical quasiparticle models [41][42][43][44], holography [45][46][47], lattice QCD [29,[48][49][50], Dyson-Schwinger calculations [51], in the Polyakov-extended quarkmeson model [52], semianalytic calculations within perturbative QCD [53][54][55], and also taking into account strong magnetic fields [56,57]. Closer to the systems we are considering in this work we mention semianalytical calculations in a pion gas using chiral perturbation theory with and without unitarization [33,58], in a pion gas using a sigma model with and without mediummodified interactions [59], in a sigma model with baryon interactions [60], and in resonance gas models [27,61].…”