Neutron Star Quantum Death by Small Black Holes

TL;DR

This paper investigates how quantum mechanical effects alter the accretion process of small black holes inside neutron stars, impacting their destruction and lifetime predictions, especially for black holes formed from dark matter collapse.

Contribution

It introduces a quantum mechanical model for black hole accretion in neutron stars, refining previous classical models and identifying the mass range where black holes can persist without rapid evaporation.

Findings

Black holes lighter than ~10^{11} kg evaporate quickly.

Black holes between 10^{11} and 10^{12} kg can survive longer, potentially destroying neutron stars.

Quantum effects significantly modify accretion rates for small black holes.

Abstract

Neutron stars can be destroyed by black holes at their center accreting material and eventually swallowing the entire star. Here we note that the accretion model adopted in the literature, based on Bondi accretion or variations thereof, is inadequate for small black holes -- black holes whose Schwarzschild radius is comparable to, or smaller than, the neutron's de Broglie wavelength. In this case, quantum mechanical aspects of the accretion process cannot be neglected, and give rise to a completely different accretion rate. We show that for the case of black holes seeded by the collapse of bosonic dark matter, this is the case for electroweak-scale dark matter particles. In the case of fermionic dark matter, typically the black holes that would form at the center of a neutron star are more massive, unless the dark matter particle mass is very large, larger than about 10$^{10}$ GeV. We calculate the lifetime of neutron stars harboring a ``small'' black hole, and find that black holes lighter than $\sim 10^{11}$ kg quickly evaporate, leaving no trace. More massive black holes destroy neutron stars via quantum accretion on time-scales much shorter than the age of observed neutron stars. We find that the range where seed black holes inside neutron stars are massive enough that they do not quickly evaporate away, but not so massive that a fluid accretion picture is warranted is limited to between $\sim10^{11}$ and $10^{12}$ kg, but our results are key to accurately determine the actual critical black hole mass corresponding to the onset of neutron star destruction