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From scalar clouds around evaporating black holes to boson star

Daniel Neves, João G. Rosa

Abstract

We study, for the first time, the evolution of a scalar cloud bound to an evaporating black hole. Our simulations of the associated Schrödinger-Poisson system for non-relativistic and spherically symmetric clouds reveal that a scalar cloud may (partially) survive as a self-gravitating boson star if the black hole evaporates adiabatically until its mass becomes less than one half of the cloud's mass. This yields a novel mechanism for boson star formation and shows that, as previously conjectured, bosonic dark matter production by light primordial black holes may result in micro-boson stars with very large occupation numbers, greatly enhancing their potential detectability even for very weakly interacting dark matter particles.

From scalar clouds around evaporating black holes to boson star

Abstract

We study, for the first time, the evolution of a scalar cloud bound to an evaporating black hole. Our simulations of the associated Schrödinger-Poisson system for non-relativistic and spherically symmetric clouds reveal that a scalar cloud may (partially) survive as a self-gravitating boson star if the black hole evaporates adiabatically until its mass becomes less than one half of the cloud's mass. This yields a novel mechanism for boson star formation and shows that, as previously conjectured, bosonic dark matter production by light primordial black holes may result in micro-boson stars with very large occupation numbers, greatly enhancing their potential detectability even for very weakly interacting dark matter particles.

Paper Structure

This paper contains 2 sections, 11 equations, 3 figures.

Table of Contents

  1. Acknowledgments

Figures (3)

  • Figure 1: Numerical evolution of the (square-root of the) particle number density (blue) for simulation A with $M_{BH,i}/M_c=5$ and $\hat{\tau}=1.5\times 10^5$. Also shown are the stationary solutions for $M_{BH}/M_c=5,2,1$ (dashed gray) and the boson star ground state solution (dashed red).
  • Figure 2: Evolution of the energy expectation value for $M_{BH,i}=5M_c$ and $\hat{\tau}=1.5\times 10^5$ (blue), compared with the energy of the boson star solution with the same mass (dashed red).
  • Figure 3: Final energy expectation value as a function of the BH-to-cloud mass ratio at the non-adiabatic point.