2005MNRAS.362.1085Q


Query : 2005MNRAS.362.1085Q

2005MNRAS.362.1085Q - Mon. Not. R. Astron. Soc., 362, 1085-1098 (2005/September-3)

Deviation of light curves of gamma-ray burst pulses from standard forms due to the curvature effect of spherical fireballs or uniform jets.

QIN Y.-P. and LU R.-J.

Abstract (from CDS):

As revealed previously, under the assumption that some pulses of gamma-ray bursts are produced by shocks in spherical fireballs or uniform jets of large opening angles, there exists a standard decay form of the profile of pulses arising from very narrow or suddenly dimming local (or intrinsic) pulses due to the relativistic curvature effect (the Doppler effect over the spherical shell surface). Profiles of pulses arising from other local pulses were previously found to possess a reverse S-feature deviation from the standard decay form. We show in this paper that, in addition to the standard decay form shown in Qin et al., there exists a marginal decay curve associated with a local δ function pulse with a monocolour radiation. We employ the sample of Kocevski, Ryde & Liang to check this prediction and find that the phenomenon of the reverse S-feature is common, when compared with both the standard decay form and the marginal decay curve. We accordingly propose to take the marginal decay curve (whose function is simple) as a criterion to check if an observed pulse could be taken as a candidate suffered from the curvature effect. We introduce two quantities A1and A2to describe the mentioned deviations within and beyond the full width at half-maximum position of the decay phase, respectively. The values of A1and A2of pulses of the sample are calculated, and the result suggests that for most of these pulses their corresponding local pulses might contain a long decay time relative to the time-scale of the curvature effect.

Abstract Copyright: 2004 RAS

Journal keyword(s): relativity - gamma-rays: bursts - gamma-rays: theory

Simbad objects: 66

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Number of rows : 66
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 3B 930909 gB 01 03.3 +36 50           ~ 14 0
2 GRB 980302 gB 01 59 -08.2           ~ 19 0
3 3B 930914 gB 02 08.8 +34 26           ~ 15 0
4 4B 941121 gB 02 21.8 -66 22           ~ 21 0
5 4B 951016 gB 02 23.3 -24 22           ~ 25 0
6 GRB 950211B gB 04 17.4 -55 01           ~ 20 0
7 GRB 990528 gB 04 30 -14.9           ~ 17 0
8 GRB 990707 gB 05 04 +24.3           ~ 15 0
9 3B 931221 gB 06 04.1 -43 10           ~ 26 0
10 4B 951228 gB 06 12.5 +28 13           ~ 21 0
11 GRB 960912 gB 06 21 +78.8           ~ 20 0
12 4B 960624 gB 06 35.8 +32 03           ~ 16 0
13 GRB 970405 gB 06 37 +22.5           ~ 13 0
14 GRB 980301 gB 06 45 -30.9           ~ 17 0
15 3B 930612 gB 06 52.3 -69 46           ~ 48 0
16 3B 940313 gB 07 17.8 -14 28           ~ 18 0
17 4B 951030B gB 07 45.8 +29 34           ~ 11 0
18 2B 921015 gB 08 12.2 +41 41           ~ 25 0
19 1B 911022 gB 08 15.6 +70 20           ~ 29 0
20 GRB 980401A gB 08 24 +15.4           ~ 16 0
21 3B 931128 gB 09 30.6 +18 13           ~ 27 0
22 4B 960530 gB 09 33.6 -53 47           ~ 31 0
23 GRB 990316 gB 10 11 -05.5           ~ 27 0
24 1B 920216 gB 10 27.7 +01 10           ~ 35 0
25 2B 920801 gB 10 31.4 +68 54           ~ 24 0
26 2B 920925 gB 10 41.0 +67 23           ~ 34 1
27 4B 951019 gB 10 46.0 -87 49           ~ 22 0
28 4B 950624 gB 11 01.5 +14 59           ~ 27 0
29 GRB 990816 gB 11 48 +07.7           ~ 18 0
30 4B 951102B gB 12 38.6 -35 14           ~ 15 0
31 3B 940830 gB 12 54.6 +25 40           ~ 20 0
32 2B 930214B gB 12 59.2 +26 46           ~ 32 0
33 GRB 000323 gB 13 04 +57.1           ~ 22 0
34 GRB 990102B gB 13 35 +03.6           ~ 14 0
35 4B 941026 gB 13 43.8 -06 32           ~ 37 0
36 1B 911104 gB 14 09.8 +35 02           ~ 39 0
37 GRB 940529C gB 14 19.4 +58 56           ~ 34 0
38 4B 960114 gB 14 24.8 -29 44           ~ 23 0
39 4B 960613 gB 14 46.8 +35 58           ~ 10 0
40 GRB 990505 gB 15 08 -52.6           ~ 14 0
41 4B 960113 gB 15 21.1 +06 12           ~ 17 0
42 GRB 971127 gB 15 32 +32.2           ~ 24 0
43 4B 970815 gB 16 06 54.0 +81 30 34           ~ 56 0
44 3B 940904 gB 16 13.5 +44 05           ~ 12 0
45 3B 931127 gB 16 43.2 -23 04           ~ 20 0
46 3B 940410 gB 16 59.6 +30 48           ~ 26 0
47 2B 920830 gB 17 14.1 -73 59           ~ 38 0
48 1B 911209 gB 17 19.9 -45 05           ~ 37 0
49 2B 930120 gB 17 25.2 +14 44           ~ 37 0
50 3B 930807 gB 18 18.0 -57 50           ~ 15 0
51 GRB 990102 gB 18 22 +39.7           ~ 25 0
52 4B 950818 gB 18 34.6 +33 52           ~ 33 0
53 GRB 990712B gB 18 46 +09.5           ~ 17 0
54 4B 951213 gB 18 55.9 -06 49           ~ 26 0
55 1B 911031 gB 18 58.2 +21 20           ~ 45 0
56 1B 911016 gB 20 01.9 -03 47           ~ 47 0
57 2B 921207 gB 20 25.3 -42 56           ~ 47 0
58 4B 960715C gB 20 52.0 +51 52           ~ 12 0
59 GRB 980718 gB 21 02 -45.6           ~ 14 0
60 1B 910721 gB 21 02.1 -14 17           ~ 33 0
61 4B 960628 gB 21 47.9 +48 17           ~ 17 0
62 GRB 970925 gB 22 02 -11.7           ~ 24 0
63 GRB 000519 gB 23 04 38.6 +01 10 17           ~ 26 0
64 4B 941023B gB 23 36.1 +56 31           ~ 18 0
65 2B 920307 gB 23 42.3 -45 09           ~ 28 0
66 2B 921218 gB 23 42.5 -55 19           ~ 16 0

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