Phase transitions between dilute and dense axion stars
arXiv:1710.06268 · doi:10.1103/PhysRevD.98.023009
Abstract
We study the nature of phase transitions between dilute and dense axion stars interpreted as self-gravitating Bose-Einstein condensates. We develop a Newtonian model based on the Gross-Pitaevskii-Poisson equations for a complex scalar field with a self-interaction potential involving an attractive term and a repulsive term. Using a Gaussian ansatz for the wave function, we analytically obtain the mass-radius relation of dilute and dense axion stars for arbitrary values of the self-interaction parameter . We show the existence of a critical point above which a first order phase transition takes place. We qualitatively estimate general relativistic corrections on the mass-radius relation of axion stars. For weak self-interactions , a system of self-gravitating axions forms a stable dilute axion star below a general relativistic maximum mass and collapses into a black hole above that mass. For strong self-interactions , a system of self-gravitating axions forms a stable dilute axion star below a Newtonian maximum mass , collapses into a dense axion star above that mass, and collapses into a black hole above a general relativistic maximum mass . Dense axion stars explode below a Newtonian minimum mass and form dilute axion stars of large size or disperse away. We determine the phase diagram of self-gravitating axions and show the existence of a triple point separating dilute axion stars, dense axion stars, and black holes. We make numerical applications for QCD axions and ultralight axions.
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