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Two Predictions of supernova: GRB 130427A / SN 2013cq and GRB 180728A / SN 2018fip

Published 13 Nov 2018 in astro-ph.HE | (1811.05433v3)

Abstract: On 2018 July 28, GRB 180728A triggered \textit{Swift} satellites and, soon after the determination of the redshift, we identified this source as a type II binary-driven hypernova (BdHN II) in our model. Consequently, we predicted the appearance time of its associated supernova (SN), which was later confirmed as SN 2018fip. A BdHN II originates in a binary composed of a carbon-oxygen core (COcore_{\rm core}) undergoing SN, and the SN ejecta hypercritically accrete onto a companion neutron star (NS). From the time of the SN shock breakout to the time when the hypercritical accretion starts, we infer the binary separation ≃3×10<sup>10\simeq 3 \times 10<sup>{10} cm. The accretion explains the prompt emission of isotropic energy ≃3×10<sup>51\simeq 3 \times 10<sup>{51} erg, lasting ∼10\sim 10 s, and the accompanying observed blackbody emission from a thermal convective instability bubble. The new neutron star (ν\nuNS) originating from the SN powers the late afterglow from which a ν\nuNS initial spin of $2.5$ ms is inferred. We compare GRB 180728A with GRB 130427A, a type I binary-driven hypernova (BdHN I) with isotropic energy $&gt; 10<sup>{54}$ erg. For GRB 130427A we have inferred an initially closer binary separation of ≃10<sup>10\simeq 10<sup>{10} cm, implying a higher accretion rate leading to the collapse of the NS companion with consequent black hole formation, and a faster, $1$ ms spinning ν\nuNS. In both cases, the optical spectra of the SNe are similar, and not correlated to the energy of the gamma-ray burst. We present three-dimensional smoothed-particle-hydrodynamic simulations and visualisations of the BdHNe I and II.

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