Structure formation during phase transitions in strongly interacting matter
arXiv:2207.03212 · doi:10.1016/j.ppnp.2023.104030
Abstract
A broad range of problems associated with phase transitions in systems characterized by the strong interaction between particles and with formation of structures is reviewed. A general phenomenological mean-field model is constructed describing phase transitions of the first and the second order to the and states. Due to fluctuations, the phase transition to the state is the transition of the first order. Various specific features of the phase transitions to the state are considered such as the anisotropic spectrum of excitations, a possibility of the formation of various structures including running and standing waves, three-axis structures, chiral waves, pasta phases, etc. A formal transition to hydrodynamical variables is performed. Then focus is made on description of the dynamics of the order parameter at the phase transitions to the states with and . Next the non-ideal hydrodynamical description of the phase transitions of the liquid-gas type in nuclear systems is performed. Quasiperiodic structures are developed. Next, pion condensation phase transition to the state in dense, cold or warm nuclear matter is considered and then the high temperature -- small baryon chemical potential system is studied, when baryons become completely blurred and light bosons, e.g., pions, may condense either in or states. Then, for scalar collective modes phenomena of the Pomeranchuk instability and the Bose condensation in or states are studied. Next, possibility of the condensation of Bose excitations in the state in moving media is considered. Then Bose-Einstein condensation of pions at dynamically fixed number of particles is studied and specific non-equilibrium effects are demonstrated on an example.
arXiv comment110pages, 13 figures
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