2016ApJ...833..110I


Query : 2016ApJ...833..110I

2016ApJ...833..110I - Astrophys. J., 833, 110-110 (2016/December-2)

Are ultra-long gamma-ray bursts caused by blue supergiant collapsars, newborn magnetars, or white dwarf tidal disruption events?

IOKA K., HOTOKEZAKA K. and PIRAN T.

Abstract (from CDS):

Ultra-long gamma-ray bursts (ulGRBs) are a new population of GRBs with extreme durations of ∼104 s. Leading candidates for their origin are blue supergiant collapsars, magnetars, and white dwarf tidal disruption events (WD-TDEs) caused by massive black holes (BHs). Recent observations of supernova-like (SN-like) bumps associated with ulGRBs challenged both the WD-TDE and the blue supergiant models because of the detection of SNe and the absence of hydrogen lines, respectively. We propose that WD-TDEs can accommodate the observed SN-like bumps if the fallback WD matter releases energy into the unbound WD ejecta. The observed ejecta energy, luminosity, and velocity are explained by the gravitational energy, Eddington luminosity, and escape velocity of the formed accretion disk, respectively. We also show that the observed X-rays can ionize the ejecta, eliminating lines. The SN-like light curves (SN 2011kl) for the ulGRB 111209A are consistent with all three models, although a magnetar model is unnatural because the spin-down time required to power the SN-like bump is a hundred times longer than the GRB. Our results imply that TDEs are a possible energy source for SN-like events in general and for ulGRBs in particular.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): black hole physics - Galaxy: nucleus - gamma-ray burst: general - gamma-ray burst: individual: GRB 111209A - stars: magnetars - supernovae: general - supernovae: general

Simbad objects: 13

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Number of rows : 13
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
3 SN 2011kg SN* 01 39 45.51 +29 55 27.0           SLSN-I 73 1
4 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
5 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
6 GRB 141121A gB 08 10 40.68 +22 13 02.7           ~ 108 0
7 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
8 PS1-11af ev 09 57 26.815 +03 14 01.00           ~ 71 0
9 SWIFT J1112.2-8238 X 11 11 47.797 -82 38 44.71           ~ 81 0
10 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
11 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
12 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0
13 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1

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