Abstract

The equation of state and phase diagram of strongly interacting matter composed of αα particles are studied in the mean-field approximation. The particle interactions are included via a Skyrme-like mean field, containing both attractive and repulsive terms. The model parameters are found by fitting known values of binding energy and baryon density in the ground state of αα matter, obtained from microscopic calculations by Clark and Wang. Thermodynamic quantities of αα matter are calculated in the broad domains of temperature and baryon density, which can be reached in heavy-ion collisions at intermediate energies. The model predicts both first-order liquid-gas phase transition and Bose-Einstein condensation of αα particles. We present the profiles of scaled variance, sound velocity and isochoric heat capacity along the isentropic trajectories of αα matter. Strong density fluctuations are predicted in the vicinity of the critical point at temperature Tc≈14 MeVT_c\approx 14~\textrm{MeV} and density nc≈0.012 fm−3n_c\approx 0.012~\textrm{fm}^{-3}.

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