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    Framework for phase transitions between the Maxwell and Gibbs constructions at finite temperature

    Constantinos Constantinou1,2,*, Mirco Guerrini3,4,†, Tianqi Zhao5,6,7,‡, Sophia Han8,9,7,10,§, and Madappa Prakash5,∥

    • *Contact author: cconstantinou@ectstar.eu
    • †Contact author: mirco.guerrini@unife.it
    • ‡Contact author: tianqi.zhao@berkeley.edu
    • §Contact author: sjhan@sjtu.edu.cn
    • ∥Contact author: prakash@ohio.edu

    Phys. Rev. D 112, 094014 – Published 10 November, 2025

    DOI: https://doi.org/10.1103/8l3m-tdlc

    Abstract

    The characteristics of the hadron-to-quark first-order phase transition differ depending on whether charge neutrality is locally or globally fulfilled. In β-equilibrated matter, these two possibilities correspond to the Maxwell and Gibbs constructions. Recently, we presented a new framework in which a continuously varying parameter allows one to describe a first-order phase transition in intermediate scenarios to the two extremes of fully local and fully global charge neutrality. In this work, we extend the previous framework to finite temperatures and out-of-β equilibrium conditions, making it available for simulations of core-collapse supernovae and binary neutron star mergers. We investigate its impact on key thermodynamic quantities across a range of baryon densities, temperatures, and electron fractions. We find that when matter is not in β equilibrium, the pressure in the mixed phase is not constant even for the case of fully local charge neutrality. Moreover, we compute the thermal index using three different approaches, demonstrating that the finite-temperature extension of an equation of state using a constant thermal index can be ill defined when applied to the mixed phase.

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