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 :
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