Literature DB >> 23630378

The long, the short and the weak: the origin of gamma-ray bursts.

Tsvi Piran1, Omer Bromberg, Ehud Nakar, Re'em Sari.   

Abstract

The origin of gamma-ray bursts (GRBs) is one of the most interesting puzzles in recent astronomy. During the last decade a consensus has formed that long GRBs (LGRBs) arise from the collapse of massive stars, and that short GRBs (SGRBs) have a different origin, most likely neutron star mergers. A key ingredient of the collapsar model that explains how the collapse of massive stars produces a GRB is the emergence of a relativistic jet that penetrates the stellar envelope. The condition that the emerging jet penetrates the envelope imposes strong constraints on the system. Using these constraints we show the following. (i) Low-luminosity GRBs (llGRBs), a subpopulation of GRBs with very low luminosities (and other peculiar properties: single-peaked, smooth and soft), cannot be formed by collapsars. llGRBs must have a different origin (most likely a shock breakout). (ii) On the other hand, regular LGRBs must be formed by collapsars. (iii) While for BATSE the dividing line between collapsars and non-collapsars is indeed at approximately 2 s, the dividing line is different for other GRB detectors. In particular, most Swift bursts longer than 0.8 s are of a collapsar origin. This last result requires a revision of many conclusions concerning the origin of Swift SGRBs, which were based on the commonly used 2 s limit.

Year:  2013        PMID: 23630378     DOI: 10.1098/rsta.2012.0273

Source DB:  PubMed          Journal:  Philos Trans A Math Phys Eng Sci        ISSN: 1364-503X            Impact factor:   4.226


  2 in total

1.  Interpreting signals from astrophysical transient experiments.

Authors:  Paul T O'Brien; Stephen J Smartt
Journal:  Philos Trans A Math Phys Eng Sci       Date:  2013-04-29       Impact factor: 4.226

Review 2.  Gamma-ray bursts and their use as cosmic probes.

Authors:  Patricia Schady
Journal:  R Soc Open Sci       Date:  2017-07-26       Impact factor: 2.963

  2 in total

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