TY - JOUR
T1 - Neutrino and cosmic-ray release from gamma-ray bursts
T2 - Time-dependent simulations
AU - Asano, Katsuaki
AU - Mészáros, Peter
PY - 2014/4/10
Y1 - 2014/4/10
N2 - We revisit the neutrino and ultra-high-energy cosmic-ray (UHECR) production from gamma-ray bursts (GRBs) with time-dependent simulations for the proton-induced cascades. This method can generate self-consistent photon, neutrino, and escaped neutron spectra. To obtain the integrated background spectra, we take into account the distributions of the burst luminosity and pulse duration timescale. A benchmark case with standard GRB luminosity function, a bulk Lorentz factor Γ = 300, and a proton to gamma-ray luminosity fraction fp = 10 is consistent with both the neutrino upper limits and the observed UHECR intensity at 1020 eV, while requiring a different type of UHECR source at the ankle. For the benchmark case, the GRBs in the bright end of the luminosity function, which contribute most of the neutrinos, have their photon spectrum substantially distorted by secondary photons. Such bright GRBs are few in number, and reducing their fp eliminates the distortion and reduces the neutrino production. Even if we neglect the contribution of the brightest GRBs, the UHECR production rate at energies corresponding to the Greisen-Zatsepin-Kuzmin limit is almost unchanged. These nominal GRB models, especially with L iso ≲ 1053 erg s -1, appear to meet the current constraints as far as being candidate UHECR sources above the ankle energy.
AB - We revisit the neutrino and ultra-high-energy cosmic-ray (UHECR) production from gamma-ray bursts (GRBs) with time-dependent simulations for the proton-induced cascades. This method can generate self-consistent photon, neutrino, and escaped neutron spectra. To obtain the integrated background spectra, we take into account the distributions of the burst luminosity and pulse duration timescale. A benchmark case with standard GRB luminosity function, a bulk Lorentz factor Γ = 300, and a proton to gamma-ray luminosity fraction fp = 10 is consistent with both the neutrino upper limits and the observed UHECR intensity at 1020 eV, while requiring a different type of UHECR source at the ankle. For the benchmark case, the GRBs in the bright end of the luminosity function, which contribute most of the neutrinos, have their photon spectrum substantially distorted by secondary photons. Such bright GRBs are few in number, and reducing their fp eliminates the distortion and reduces the neutrino production. Even if we neglect the contribution of the brightest GRBs, the UHECR production rate at energies corresponding to the Greisen-Zatsepin-Kuzmin limit is almost unchanged. These nominal GRB models, especially with L iso ≲ 1053 erg s -1, appear to meet the current constraints as far as being candidate UHECR sources above the ankle energy.
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U2 - 10.1088/0004-637X/785/1/54
DO - 10.1088/0004-637X/785/1/54
M3 - Article
AN - SCOPUS:84897378956
SN - 0004-637X
VL - 785
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 54
ER -