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The lowest-mass stellar black holes: catastrophic death of neutron stars in gamma-ray bursts

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arxiv 0712.1036 v2 pith:REZP4IQX submitted 2007-12-06 astro-ph

classification astro-ph
keywords neutronstargamma-rayblackburstsdoubleholemass
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Mergers of double neutron stars are considered the most likely progenitors for short gamma-ray bursts. Indeed such a merger can produce a black hole with a transient accreting torus of nuclear matter (Lee & Ramirez-Ruiz 2007, Oechslin & Janka 2006), and the conversion of a fraction of the torus mass-energy to radiation can power a gamma-ray burst (Nakar 2006). Using available binary pulsar observations supported by our extensive evolutionary calculations of double neutron star formation, we demonstrate that the fraction of mergers that can form a black hole -- torus system depends very sensitively on the (largely unknown) maximum neutron star mass. We show that the available observations and models put a very stringent constraint on this maximum mass under the assumption that a black hole formation is required to produce a short gamma-ray burst in a double neutron star merger. Specifically, we find that the maximum neutron star mass must be within 2 - 2.5 Msun. Moreover, a single unambiguous measurement of a neutron star mass above 2.5 Msun would exclude a black hole -- torus central engine model of short gamma-ray bursts in double neutron star mergers. Such an observation would also indicate that if in fact short gamma-ray bursts are connected to neutron star mergers, the gamma-ray burst engine is best explained by the lesser known model invoking a highly magnetized massive neutron star (e.g., Usov 1992; Kluzniak & Ruderman 1998; Dai et al. 2006; Metzger, Quataert & Thompson 2007).

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  1. Connecting GRBs from Binary Neutron Star Mergers to Nuclear Properties of Neutron Stars

    astro-ph.HE 2024-12 conditional novelty 6.0 of 10

    By matching population-synthesis predictions to the observed ratio of long to short GRBs from binary neutron star mergers, the authors infer that the long-short remnant transition lies near M_ls ~ 1.3 M_TOV.

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