2002A&A...393L..15M


Query : 2002A&A...393L..15M

2002A&A...393L..15M - Astronomy and Astrophysics, volume 393, L15-19 (2002/10-1)

Kerr black holes and time profiles of gamma ray bursts.

McBREEN S., McBREEN B., HANLON L. and QUILLIGAN F.

Abstract (from CDS):

The cumulative light curves of Gamma Ray Bursts (GRBs) smooth the spiky nature of the running light curve. The cumulative count increases in an approximate linear way with time t for most bursts. In 19 out of 398 GRBs with T90>2s, the cumulative light curve was found to increase with time as ∼t2 implying a linear increase in the running light curve. The non-linear sections last for a substantial fraction of the GRB duration, have a large proportion of the cumulative count and many resolved pulses that usually end with the highest pulse in the burst. The reverse behaviour was found in 11 GRBs where the running light curve decreased with time and some bursts are good mirror images of the increases. These GRBs are among the spectrally hardest bursts observed by BATSE. The most likely interpretation is that these effects are signatures of black holes that are either being spun up or down in the accretion process. In the spin up case, the increasing Kerr parameter of the black hole allows additional rotational and accretion energy to become available for extraction. The process is reversed if the black hole is spun down by magnetic field torques. The luminosity changes in GRBs are consistent with the predictions of the BZ process and neutrino annihilation and thus provide the link to spinning black holes. GRBs provide a new window for studying the general relativistic effects of Kerr black holes.

Abstract Copyright:

Journal keyword(s): gamma rays - bursts: gamma rays - observations: methods - data analysis: methods - statistical

Simbad objects: 30

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Number of rows : 30
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 960703B gB 00 18.5 -07 45           ~ 13 0
2 GRB 980203 gB 00 22 -15.1           ~ 13 0
3 3B 930720 gB 01 23.3 +25 20           ~ 17 0
4 1B 910619 gB 01 24.7 -36 34           ~ 23 0
5 4B 951011 gB 02 43.4 -57 35           ~ 13 0
6 GRB 990111A gB 02 57 +35.5           ~ 10 0
7 4B 941018 gB 03 43.0 -16 17           ~ 9 0
8 GRB 980208 gB 04 00 -76.8           ~ 11 0
9 GRB 940526B gB 05 21.6 -30 23           ~ 18 0
10 4B 950401B gB 05 44.2 +43 45           ~ 15 0
11 GRB 970831 gB 05 49 -47.8           ~ 12 0
12 GRB 971029 gB 06 38 +28.4           ~ 15 0
13 GRB 990915 gB 06 38 +75.7           ~ 13 0
14 3B 940526 gB 08 47.4 +34 12           ~ 26 0
15 GRB 980803 gB 10 04 +58.0           ~ 12 0
16 3B 940414 gB 12 05.0 -26 09           ~ 19 0
17 3B 940323 gB 14 15.6 +08 22           ~ 20 0
18 4B 951219 gB 16 03.2 +60 31           ~ 13 0
19 1B 911127 gB 17 56.6 +49 44           ~ 36 0
20 1B 920226 gB 18 05.0 +17 28           ~ 29 0
21 3B 940803B gB 18 23.4 -06 56           ~ 10 0
22 GRB 990718 gB 18 59 +01.0           ~ 8 0
23 GRB 980420 gB 19 31.2 +26 34           ~ 10 0
24 3B 940619 gB 19 56.2 -29 53           ~ 24 0
25 Trigger 6903 gB 20 05 +32.8           ~ 4 0
26 3B 940520 gB 21 34.0 +06 56           ~ 20 0
27 GRB 000511A gB 22 16 -38.3           ~ 10 0
28 4B 950208 gB 22 27.8 +54 11           ~ 21 0
29 1B 910814 gB 23 05.4 +30 26           ~ 80 0
30 GRB 990518 gB 23 16 -37.1           ~ 13 0

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