2016ApJ...833..129X


Query : 2016ApJ...833..129X

2016ApJ...833..129X - Astrophys. J., 833, 129-129 (2016/December-3)

Numerical and analytical solutions of neutrino-dominated accretion flows with a non-zero torque boundary condition and its applications in gamma-ray bursts.

XIE W., LEI W.-H. and WANG D.-X.

Abstract (from CDS):

A stellar-mass black hole (BH) surrounded by a neutrino-dominated accretion flow (NDAF) has been discussed in a number of works as the central engine of gamma-ray bursts (GRBs). It is widely believed that NDAF cannot liberate enough energy for bright GRBs. However, these works have been based on the assumption of a "no torque" boundary condition, which is invalid when the disk is magnetized. In this paper, we present both numerical and analytical solutions for NDAFs with non-zero boundary stresses and reexamine their properties. We find that an NDAF with such a boundary torque can be powerful enough to account for those bright short GRBs, energetic long GRBs, and ultra-long GRBs. The disk becomes viscously unstable, which makes it possible to interpret the variability of GRB prompt emission and the steep decay phase in the early X-ray afterglow. Finally, we study the gravitational waves radiated from a processing BH-NDAF. We find that the effects of the boundary torque on the strength of the gravitational waves can be ignored.

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

Journal keyword(s): accretion, accretion disks - gamma-ray burst: general - magnetic fields - neutrinos - neutrinos

Simbad objects: 17

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Number of rows : 17
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 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
3 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
4 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
5 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
6 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
7 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
8 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
9 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
10 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
11 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
12 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
13 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
14 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
15 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
16 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
17 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0

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