2013ApJ...768..187B


Query : 2013ApJ...768..187B

2013ApJ...768..187B - Astrophys. J., 768, 187 (2013/May-2)

A new method of pulse-wise spectral analysis of gamma-ray bursts.

BASAK R. and RAO A.R.

Abstract (from CDS):

Time-resolved spectral analysis, though a very promising method to understand the emission mechanism of gamma-ray bursts (GRBs), is difficult to implement in practice because of poor statistics. We present a new method for pulse-wise time-resolved spectral study of the individual pulses of GRBs, using the fact that many spectral parameters are either constants or smooth functions of time. We use this method for the two pulses of GRB 081221, the brightest GRB with separable pulses. We choose, from the literature, a set of possible models that includes the Band model, blackbody with a power law (BBPL), and a collection of blackbodies with a smoothly varying temperature profile, along with a power law (mBBPL), and two blackbodies with a power law (2BBPL). First, we perform a time-resolved study to confirm the spectral parameter variations, and then we construct the new model to perform a joint spectral fit. We find that any photospheric emission in terms of blackbodies is required mainly in the rising parts of the pulses and the falling part can be adequately explained in terms of the Band model, with the low-energy photon index within the regime of synchrotron model. Interestingly, we find that 2BBPL is comparable or sometimes even better, though marginally, than the Band model, in all episodes. Consistent results are also obtained for the brightest GRB of Fermi era–GRB 090618. We point out that the method is generic enough to test any spectral model with well-defined parameter variations.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - methods: data analysis - methods: observational

Simbad objects: 16

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Number of rows : 16
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 041006 gB 00 54 50.17 +01 14 07.0           ~ 202 2
2 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
3 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
4 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
5 GRB 081118 gB 05 30 22.28 -43 18 03.1           ~ 79 0
6 Fermi bn080925775 gB 06 24.4 +18 12           ~ 28 0
7 GRB 081207 gB 07 29.6 +70 30           ~ 26 0
8 Fermi bn081217983 gB 07 47.2 +26 48           ~ 15 0
9 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
10 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
11 Fermi bn080904886 gB 14 16.8 -30 18           ~ 18 0
12 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
13 Fermi bn090129880 gB 17 56 25.10 -32 47 34.8           ~ 36 0
14 GRB 090709A gB 19 19 46.70 +60 43 40.8           ~ 125 0
15 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
16 GRB 981021 gB 23 47 +01.0           ~ 14 0

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