4.2 Article

Bounding the time delay between high-energy neutrinos and gravitational-wave transients from gamma-ray bursts

期刊

ASTROPARTICLE PHYSICS
卷 35, 期 1, 页码 1-7

出版社

ELSEVIER
DOI: 10.1016/j.astropartphys.2011.04.001

关键词

Gravitational wave; High-energy neutrino; Gamma-ray burst; Multimessenger; Time window

资金

  1. National Science Foundation [PHY-0847182]
  2. Swedish Research Council (VR)
  3. French Agence Nationale de la Recherche [ANR-08-JCJC-0061-01]
  4. EU
  5. Direct For Mathematical & Physical Scien
  6. Division Of Physics [847182] Funding Source: National Science Foundation
  7. Direct For Mathematical & Physical Scien
  8. Division Of Physics [0757058] Funding Source: National Science Foundation
  9. Agence Nationale de la Recherche (ANR) [ANR-08-JCJC-0061] Funding Source: Agence Nationale de la Recherche (ANR)

向作者/读者索取更多资源

We derive a conservative coincidence time window for joint searches of gravitational-wave (GW) transients and high-energy neutrinos (HENS, with energies greater than or similar to 100 GeV), emitted by gamma-ray bursts (GRBs). The last are among the most interesting astrophysical sources for coincident detections with current and near-future detectors. We take into account a broad range of emission mechanisms. We take the upper limit of GRB durations as the 95% quantile of the T90's of GRBs observed by BATSE, obtaining a GRB duration upper limit of similar to 150 s. Using published results on high-energy (>100 MeV) photon light curves for 8 GRBs detected by Fermi LAT, we verify that most high-energy photons are expected to be observed within the first similar to 150 s of the GRB. Taking into account the breakout-time of the relativistic jet produced by the central engine, we allow GW and HEN emission to begin up to 100 s before the onset of observable gamma photon production. Using published precursor time differences, we calculate a time upper bound for precursor activity, obtaining that 95% of precursors occur within similar to 250 s prior to the onset of the GRB. Taking the above different processes into account, we arrive at a time window of t(HEN) - t(GW) is an element of [-500 s,+500 s]. Considering the above processes, an upper bound can also be determined for the expected time window of GW and/or HEN signals coincident with a detected GRB, t(GW) - t(GRB) approximate to t(HEN) - t(GRB) is an element of [-350 s, +150 s]. These upper bounds can be used to limit the coincidence time window in multimessenger searches, as well as aiding the interpretation of the times of arrival of measured signals. (C) 2011 Elsevier B.V. All rights reserved.

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