4.6 Article

Stringent Search for Precursor Emission in Short GRBs from Fermi/GBM Data and Physical Implications

期刊

ASTROPHYSICAL JOURNAL LETTERS
卷 902, 期 2, 页码 -

出版社

IOP Publishing Ltd
DOI: 10.3847/2041-8213/abbfb8

关键词

Gamma-ray bursts; Neutron stars; Gravitational waves; Astrostatistics

资金

  1. China Postdoctoral Science Foundation [2018M642000, 2019T120335]
  2. Fundamental Research Funds for the Central Universities [14380035]
  3. National Key Research and Development Programs of China [2018YFA0404204]
  4. National Natural Science Foundation of China [11833003]

向作者/读者索取更多资源

We perform a stringent search for precursor emission of short gamma-ray bursts (SGRBs) from the Fermi/GBM data and find 16 precursor events with greater than or similar to 4.5 sigma significance. We find that the durations of the main SGRB emission (T-GRB) and the precursor emission (T-pre), as well as the waiting time (T-wt) in between, are roughly comparable to each other, with T-wt approximate to 2.8 T-GRB(1.2) approximately satisfied for most cases except one significant outlier. We also perform spectral analyses to the precursors and SGRBs, and find that the spectra of precursor emission can be fitted with the blackbody, nonthermal cutoff power law and/or power-law models. We consider several possible models for precursor emission in SGRBs and find that the luminosity and spectral shape may be explained by the the shock breakout or the photospheric radiation of a fireball launched after the merger for thermal precursors, or magnetospheric interaction between two neutron stars prior to the merger for nonthermal precursors. For the fireball photospheric model, a matter-dominated jet is preferred and a constraint on the fireball Lorentz factor can be placed as Gamma similar to 30. For the magnetospheric interaction model, the jet launching mechanism may be constrained. In particular, those events with T-wt/T-GRB >> 1 (e.g., GRB191221802) require the formation of a supramassive or stable neutron star after the merger, with the delay time defined by the timescale for an initially baryon-loaded jet to become magnetically dominated and relativistic.

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