2022
DOI: 10.1051/0004-6361/202140403
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Radio data challenge the broadband modelling of GRB 160131A afterglow

Abstract: Context. Gamma-ray burst (GRB) afterglows originate from the interaction between the relativistic ejecta and the surrounding medium. Consequently, their properties depend on several aspects: radiation mechanisms, relativistic shock micro-physics, circumburst environment, and the structure and geometry of the relativistic jet. While the standard afterglow model accounts for the overall spectral and temporal evolution for a number of GRBs, its validity limits emerge when the data set is particularly rich and con… Show more

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Cited by 3 publications
(2 citation statements)
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References 162 publications
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“…There are also a few GRBs with radio afterglow evolution that deviates from the expected reverse-forward external shock framework for which ISS may not be the only explanation. A detailed radio analysis of GRB 160131A by Marongiu et al (2022) detected several spectral peaks (the most consistent at 8 GHz) in its radio spectra between 0.8 and 25 days post-burst that could be due to ISS, a two-component jet (e.g van der Horst et al 2014), or a thermally emitting population of electrons (Eichler & Waxman 2005). Such a thermal population would be the fraction of electrons not accelerated into a power law distribution by the shock and may result in an early radio "pre-brightening" (Eichler & Waxman 2005;Giannios & Spitkovsky 2009;Ressler & Laskar 2017).…”
mentioning
confidence: 99%
“…There are also a few GRBs with radio afterglow evolution that deviates from the expected reverse-forward external shock framework for which ISS may not be the only explanation. A detailed radio analysis of GRB 160131A by Marongiu et al (2022) detected several spectral peaks (the most consistent at 8 GHz) in its radio spectra between 0.8 and 25 days post-burst that could be due to ISS, a two-component jet (e.g van der Horst et al 2014), or a thermally emitting population of electrons (Eichler & Waxman 2005). Such a thermal population would be the fraction of electrons not accelerated into a power law distribution by the shock and may result in an early radio "pre-brightening" (Eichler & Waxman 2005;Giannios & Spitkovsky 2009;Ressler & Laskar 2017).…”
mentioning
confidence: 99%
“…Clearly, ò e < 1, but its value is not entirely certain. Studies of gamma-ray afterglows, for example, find ò e ∼ 0.1 (Panaitescu & Kumar 2002; Yost et al 2003;Chevalier et al 2004;Marongiu et al 2022). Simulations of particle acceleration in shocks also find that about 10% of the post-shock energy is in relativistic ions (Caprioli & Spitkovsky 2014), so, if electrons and ions equilibrate, then ò e ∼ 0.1; however, in low-density winds it is unlikely that they do equilibrate, which would suggest ò e = 0.1.…”
Section: Electron Distributionmentioning
confidence: 99%