1990
DOI: 10.1103/physrevd.41.3052
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Quark- and gluon-jet emission from primordial black holes: The instantaneous spectra

Abstract: We investigate the emission of quark and gluon jets from black holes with temperatures of 0.02-100 GeV, by convolving the Hawking emission formulas with a Monte Carlo QCD jet code. Jet emission may be astrophysically important particularly if black holes form from initial density perturbations in the early Universe. We find that the total emission differs dramatically from previous calculations and is dominated by the jet fragmentation products. The spectra have a significant component at energies well below t… Show more

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Cited by 321 publications
(470 citation statements)
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“…The photons which are directly radiated (not the result of decay of other primary particles) are visible as a much smaller peak at a much higher photon energy proportional to the black hole temperature [11]. As the evaporation proceeds to higher temperatures, the greater will be the number of emitted fundamental particle degrees of freedom.…”
Section: Primordial Black Hole Burst Spectrummentioning
confidence: 99%
“…The photons which are directly radiated (not the result of decay of other primary particles) are visible as a much smaller peak at a much higher photon energy proportional to the black hole temperature [11]. As the evaporation proceeds to higher temperatures, the greater will be the number of emitted fundamental particle degrees of freedom.…”
Section: Primordial Black Hole Burst Spectrummentioning
confidence: 99%
“…Here x φ denotes the fraction of PBH luminosity |dM/dt ′ | carried away by moduli; for the MSSM content, x φ ≃ 6 × 10 −3 for s = 0 with one degree of freedom (e.g., a modulus field), x φ ≃ 6 × 10 −3 for s = 1/2 with two degrees of freedom (e.g., helicity ±1/2 states of the gravitino), and x φ ≃ 9×10 −4 for s = 3/2 with 2 degrees of freedom (e.g., helicity ±3/2 states of the gravitino) [11] (see also previous footnote). The δ distribution can be rewritten as a function of t, using the identity: δ[f (t)] = |df /dt| −1 δ(t − t s ), where t s is such that f (t s ) = 0 (here t s is uniquely and implicitly defined in terms of k, k ′ ).…”
mentioning
confidence: 99%
“…[11] for other spins, while the fraction of luminosity emitted in spin s = 3/2 (noted x φ in the following) is given in Ref. [11].…”
mentioning
confidence: 99%
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