2005ApJ...632.1008Q


Query : 2005ApJ...632.1008Q

2005ApJ...632.1008Q - Astrophys. J., 632, 1008-1020 (2005/October-3)

Relationship between the gamma-ray burst pulse width and energy due to the Doppler effect of fireballs.

QIN Y.-P., DONG Y.-M., LU R.-J., ZHANG B.-B. and JIA L.-W.

Abstract (from CDS):

We study in detail how the pulse width of gamma-ray bursts is related to energy under the assumption that the sources concerned are in the fireball stage. Due to the Doppler effect of fireballs, there exists a power-law relationship between the two quantities within a limited range of frequency. The power-law range and power-law index depend strongly on the observed peak energy Epas well as the rest-frame radiation form, and the upper and lower limits of the power-law range can be determined by Ep. It is found that within the same power-law range, the ratio of the FWHM of the rising portion to that of the decaying phase of the pulses is also related to energy in the form of power laws. A plateau/power law/plateau feature is observed in the two relationships. In the case of an obvious softening of the rest-frame spectrum, the two power-law relationships also exist, but the feature evolves to a peaked one. Predictions of the relationships in the energy range covering both the BATSE and Swift bands for a typical hard burst and a typical soft one are made. A sample of FRED (fast rise and exponential decay) pulse bursts shows that 27 out of the 28 sources belong to either the plateau/power law/plateau feature class or to the peaked feature group, suggesting that the effect concerned is indeed important for most of the sources of the sample. Among these bursts, many might undergo an obvious softening evolution of the rest-frame spectrum.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts - Gamma Rays: Theory - Relativity

Simbad objects: 28

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Number of rows : 28
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 4B 951016 gB 02 23.3 -24 22           ~ 25 0
2 4B 951228 gB 06 12.5 +28 13           ~ 21 0
3 4B 960624 gB 06 35.8 +32 03           ~ 16 0
4 3B 930612 gB 06 52.3 -69 46           ~ 48 0
5 3B 940313 gB 07 17.8 -14 28           ~ 18 0
6 4B 951030B gB 07 45.8 +29 34           ~ 11 0
7 1B 911022 gB 08 15.6 +70 20           ~ 29 0
8 3B 931128 gB 09 30.6 +18 13           ~ 27 0
9 4B 960530 gB 09 33.6 -53 47           ~ 31 0
10 1B 920216 gB 10 27.7 +01 10           ~ 35 0
11 2B 920801 gB 10 31.4 +68 54           ~ 24 0
12 2B 920925 gB 10 41.0 +67 23           ~ 34 1
13 4B 951019 gB 10 46.0 -87 49           ~ 22 0
14 4B 951102B gB 12 38.6 -35 14           ~ 15 0
15 3B 940830 gB 12 54.6 +25 40           ~ 20 0
16 4B 960613 gB 14 46.8 +35 58           ~ 10 0
17 3B 940904 gB 16 13.5 +44 05           ~ 12 0
18 3B 940410 gB 16 59.6 +30 48           ~ 26 0
19 2B 920830 gB 17 14.1 -73 59           ~ 38 0
20 3B 930807 gB 18 18.0 -57 50           ~ 15 0
21 4B 951213 gB 18 55.9 -06 49           ~ 26 0
22 1B 911031 gB 18 58.2 +21 20           ~ 45 0
23 1B 911016 gB 20 01.9 -03 47           ~ 47 0
24 2B 921207 gB 20 25.3 -42 56           ~ 47 0
25 4B 960715C gB 20 52.0 +51 52           ~ 12 0
26 4B 960628 gB 21 47.9 +48 17           ~ 17 0
27 2B 920307 gB 23 42.3 -45 09           ~ 28 0
28 2B 921218 gB 23 42.5 -55 19           ~ 16 0

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