2012ApJ...756..112L


Query : 2012ApJ...756..112L

2012ApJ...756..112L - Astrophys. J., 756, 112 (2012/September-2)

A comprehensive analysis of Fermi gamma-ray burst data. II. Ep evolution patterns and implications for the observed spectrum-luminosity relations.

LU R.-J., WEI J.-J., LIANG E.-W., ZHANG B.-B., LU H.-J., LU L.-Z., LEI W.-H. and ZHANG B.

Abstract (from CDS):

We present a time-resolved spectral analysis of 51 long and 11 short bright gamma-ray bursts (GRBs) observed with the Fermi/Gamma-Ray Burst Monitor, paying special attention to Ep evolution within each burst. Among eight single-pulse long GRBs, five show an evolution from hard to soft, while three show intensity tracking. The multi-pulse long GRBs have more complicated patterns. Statistically, the hard-to-soft evolution pulses tend to be more asymmetric than the intensity-tracking ones, with a steeper rising wing than the falling wing. Short GRBs have Ep tracking intensity exclusively with the 16 ms time-resolution analysis. We performed a simulation analysis and suggest that for at least some bursts, the late intensity-tracking pulses could be a consequence of overlapping hard-to-soft pulses. However, the fact that the intensity-tracking pattern exists in the first pulse of the multi-pulse long GRBs and some single-pulse GRBs, suggests that intensity tracking is an independent component, which may operate in some late pulses as well. For the GRBs with measured redshifts, we present a time-resolved Ep- L_γ, iso_ correlation analysis and show that the scatter of the correlation is comparable to that of the global Amati/Yonetoku relation. We discuss the predictions of various radiation models regarding Epevolution, as well as the possibility of a precessing jet in GRBs. The data pose a great challenge to each of these models, and hold the key to unveiling the physics behind GRB prompt emission.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - methods: statistical - radiation mechanisms: non-thermal

VizieR on-line data: <Available at CDS (J/ApJ/756/112): grb.dat table1.dat>

Simbad objects: 67

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Number of rows : 67
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 Fermi bn090227772 gB 00 47 +32.2           ~ 53 0
2 GRB 090922A gB 00 52.4 +74 00           ~ 26 0
3 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
5 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
6 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
7 GRB 101014A gB 01 47.8 -51 04           ~ 31 0
8 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
9 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
10 GRB 081125 gB 02 51 -18.9           ~ 30 0
11 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
12 Fermi bn100701490 gB 02 52 -02.2           ~ 20 0
13 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
14 Fermi bn081107321 gB 03 24.0 +17 06           ~ 21 0
15 GRB 100612A gB 04 14 +13.7           ~ 17 0
16 Fermi bn090530760 gB 04 53 +13.8           ~ 22 0
17 Fermi bn100122616 gB 05 16.8 -02 43           ~ 26 0
18 GRB 090820 gB 05 51 +27.1           ~ 44 0
19 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
20 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
21 GRB 090809B gB 06 21 +00.2           ~ 30 0
22 GRB 090228 gB 07 07.2 -24 18           ~ 45 0
23 GRB 081207 gB 07 29.6 +70 30           ~ 26 0
24 GRB 110529A gB 07 53.3 +67 55           ~ 27 0
25 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
26 GRB 090828 gB 08 18 -26.1           ~ 17 0
27 GRB 081215A gB 08 22 +54.0           ~ 57 0
28 Fermi bn081216531 gB 08 37 +07.6           ~ 35 0
29 Fermi bn090804940 gB 08 42 -11.3           ~ 21 0
30 GRB 101123A gB 08 45.0 +06 31           ~ 27 0
31 GRB 090305B gB 09 00.0 +74 18           ~ 22 0
32 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
33 GRB 110705A gB 10 24 +40.1           ~ 22 0
34 Fermi bn090330279 gB 10 40.8 -08 12           ~ 19 0
35 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
36 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
37 GRB 090308 gB 12 14 10.70 -48 45 13.8           ~ 28 0
38 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
39 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
40 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
41 GRB 081224 gB 14 12 35.85 +74 11 59.5           ~ 27 0
42 GRB 091120 gB 15 07.2 -21 47           ~ 34 0
43 GRB 110301A gB 15 17.4 +29 24           ~ 53 0
44 GRB 080825C gB 15 28.8 -04 54           ~ 71 0
45 GRB 090305 G 16 07 07.5960 -31 33 22.540           ~ 53 0
46 Fermi bn110123804 gB 16 28 +28.0           ~ 13 0
47 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
48 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
49 Fermi bn090108020 gB 17 23 +46.0           ~ 23 0
50 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
51 Fermi bn090718762 gB 18 16 -36.4           ~ 21 0
52 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
53 Fermi bn090902401 gB 19 24 +53.1           ~ 22 0
54 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
55 Fermi bn100116897 gB 20 20 +14.4           ~ 42 0
56 GRB 100528A gB 20 44 29 +27 48.6           ~ 37 0
57 GRB 101023A gB 21 11 51.26 -65 23 17.7           ~ 71 0
58 Fermi bn090829672 gB 21 56.8 -34 12           ~ 30 0
59 Fermi bn090524346 gB 21 58 -67.4           ~ 20 0
60 GRB 110721A gB 22 10 -38.6           ~ 155 0
61 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
62 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
63 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
64 GRB 090719 gB 22 45 -67.9           ~ 41 0
65 Fermi bn100707032 gB 23 24 -06.6           ~ 44 0
66 GRB 090131 gB 23 29.2 +21 12           ~ 37 0
67 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0

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