In a unified hadron-parton model of QCD, the hadron gas alone has a negative squared speed of sound above the chiral crossover, so partonic degrees of freedom must be excited immediately after the transition.
Cluster virial expansion for nuclear matter within a quasiparticle statistical approach
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abstract
Correlations in interacting many-particle systems can lead to the formation of clusters, in particular bound states and resonances. Systematic quantum statistical approaches allow to combine the nuclear statistical equilibrium description (law of mass action) with mean-field concepts. A chemical picture, which treats the clusters as distinct entities, serves as an intuitive concept to treat the low-density limit. Within a generalized Beth-Uhlenbeck approach, the quasiparticle virial expansion is extended to include arbitrary clusters, where special attention must be paid to avoid inconsistencies such as double counting. Correlations are suppressed with increasing density due to Pauli blocking. The contribution of the continuum to the virial coefficients can be reduced by considering clusters explicitly and introducing quasiparticle energies. The cluster-virial expansion for nuclear matter joins known benchmarks at low densities with those near saturation density.
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Speed of sound of QCD matter at chiral crossover
In a unified hadron-parton model of QCD, the hadron gas alone has a negative squared speed of sound above the chiral crossover, so partonic degrees of freedom must be excited immediately after the transition.