Title of article
Bounding the time delay between high-energy neutrinos and gravitational-wave transients from gamma-ray bursts
Author/Authors
Baret، نويسنده , , Bruny and Bartos، نويسنده , , Imre and Bouhou، نويسنده , , Boutayeb and Corsi، نويسنده , , Giancarlo Avena and Alessandra De Palma، نويسنده , , Irene Di and Donzaud، نويسنده , , Corinne and Elewyck، نويسنده , , Véronique Van and Finley، نويسنده , , Chad and Jones، نويسنده , , Gareth and Kouchner، نويسنده , , Antoine and Mلrka، نويسنده , , Szabolcs and Mلrka، نويسنده , , Zsuzsa and Moscoso، نويسنده , , Luciano and Chassande-Mottin، نويسنده , , Eric B. Papa، نويسنده , , Maria Alessandra and Pradier، نويسنده , , Thierry and Raffai، نويسنده , , Peter and Rollins، نويسنده , , Jameson and Sutton، نويسنده , , Patrick، نويسنده ,
Issue Information
روزنامه با شماره پیاپی سال 2011
Pages
7
From page
1
To page
7
Abstract
We derive a conservative coincidence time window for joint searches of gravitational-wave (GW) transients and high-energy neutrinos (HENs, with energies ≳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 ∼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 ∼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 ∼250 s prior to the onset of the GRB. Taking the above different processes into account, we arrive at a time window of tHEN − tGW ∈ [−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, tGW − tGRB ≈ tHEN − tGRB ∈ [−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.
Keywords
Time window , Gravitational wave , High-energy neutrino , Gamma-ray burst , Multimessenger
Journal title
Astroparticle Physics
Serial Year
2011
Journal title
Astroparticle Physics
Record number
1336073
Link To Document