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Compact Binary Progenitors of Short Gamma-Ray Bursts

  • Authors: Bruno Giacomazzo, Rosalba Perna, Luciano Rezzolla, Eleonora Troja, and Davide Lazzati

Giacomazzo et al. 2013 The Astrophysical Journal Letters 762 L18.

  • Provider: AAS Journals

Caption: Figure 1.

Left panel: M torus/ M as a function of the mass ratio q and of the ratio between the gravitational mass of the binary and the maximum mass for an isolated NS ( M BNS/ M max). M torus has been computed using Equation (2). The dotted lines are the isocontours corresponding to the M torus values in Table 1. Right panel: plot of M torus as a function of M BNS/ M max for all the equal-mass ( q = 1) simulations reported in Table 2. The horizontal bars give the percentage of the SGRBs in Table 1 that are generated by tori with that range of masses (assuming a total efficiency epsilon of 5% as in Table 1). Since the mass of the torus increases for q < 1, each point should be considered as a lower limit on the mass that can be obtained for that EOS and mass of the binary. The different points refer to M torus computed from simulations of BNS mergers using different EOSs (see Table 2).

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