2018ApJ...865..153L


Query : 2018ApJ...865..153L

2018ApJ...865..153L - Astrophys. J., 865, 153-153 (2018/October-1)

A comprehensive analysis of Fermi Gamma-ray Burst data. IV. Spectral lag and its relation to Ep evolution.

LU R.-J., LIANG Y.-F., LIN D.-B., LU J., WANG X.-G., LU H.-J., LIU H.-B., LIANG E.-W. and ZHANG B.

Abstract (from CDS):

The spectral evolution and spectral lag behavior of 92 bright pulses from 84 gamma-ray bursts observed by the Fermi Gamma-ray Burst Monitor (GBM) telescope are studied. These pulses can be classified into hard-to-soft pulses (H2S; 64/92), H2S-dominated-tracking pulses (21/92), and other tracking pulses (7/92). We focus on the relationship between spectral evolution and spectral lags of H2S and H2S-dominated-tracking pulses. The main trend of spectral evolution (lag behavior) is estimated with logEp∝kElog(t+t0) (1∝k1logE), where Ep is the peak photon energy in the radiation spectrum, t + t0 is the observer time relative to the beginning of pulse -t0, and 1is the spectral lag of photons with energy E with respect to the energy band 8-25 keV. For H2S and H2S-dominated-tracking pulses, a weak correlation between k1/W and kE is found, where W is the pulse width. We also study the spectral lag behavior with peak time tpE_ of pulses for 30 well-shaped pulses and estimate the main trend of the spectral lag behavior with logtpE_∝ktp_logE. It is found that ktp_ is correlated with kE. We perform simulations under a phenomenological model of spectral evolution, and find that these correlations are reproduced. We then conclude that spectral lags are closely related to spectral evolution within the pulse. The most natural explanation of these observations is that the emission is from the electrons in the same fluid unit at an emission site moving away from the central engine, as expected in the models invoking magnetic dissipation in a moderately high-σ outflow.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma-ray burst: general - methods: statistical

VizieR on-line data: <Available at CDS (J/ApJ/865/153): pulses.dat table1.dat table2.dat table3.dat table4.dat>

Simbad objects: 84

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Number of rows : 84
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 150306A gB 00 02 -58.5           ~ 9 0
2 GRB 111017A gB 00 32 -07.0           ~ 16 0
3 GRB 090922A gB 00 52.4 +74 00           ~ 26 0
4 Fermi bn110605183 gB 01 00 +52.5           ~ 11 0
5 Fermi bn110505203 gB 01 07 -32.3           ~ 8 0
6 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
7 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
8 Fermi bn141004150 gB 02 02 -77.3           ~ 3 0
9 GRB 120308B gB 02 03 +55.2           ~ 11 0
10 Fermi bn120727681 gB 02 31 +16.4           ~ 4 0
11 Fermi bn120412920 gB 02 36 +07.1           ~ 11 0
12 GRB 081125 gB 02 51 -18.9           ~ 30 0
13 Fermi bn121223300 gB 03 20 +21.4           ~ 4 0
14 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
15 Fermi bn120625119 gB 03 25 +51.1           ~ 10 0
16 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
17 GRB 110521B gB 03 50 -62.3           ~ 10 0
18 GRB 141229A gB 04 49 42.8 -19 13 58           ~ 18 0
19 Fermi bn090530760 gB 04 53 +13.8           ~ 22 0
20 GRB 120206A gB 04 54 +58.4           ~ 9 0
21 Fermi bn150514774 gB 04 59 30.45 -60 58 07.0           ~ 51 0
22 Fermi bn100122616 gB 05 16.8 -02 43           ~ 26 0
23 Fermi bn140209313 gB 05 25 19.00 +32 29 56.1           ~ 47 0
24 Fermi bn101126198 gB 05 39 -22.6           ~ 18 0
25 Fermi bn131216081 gB 06 06 -35.5           ~ 11 0
26 GRB 090809B gB 06 21 +00.2           ~ 30 0
27 Fermi bn120921877 gB 06 26 -64.8           ~ 7 0
28 Fermi bn141222691 gB 06 30 +40.1           ~ 4 0
29 Fermi bn130701060 gB 06 31 -60.1           ~ 8 0
30 GRB 140213A gB 07 00 37.18 -73 08 14.1           ~ 102 0
31 Fermi bn120426090 gB 07 26 -65.6           ~ 17 0
32 Fermi bn130815660 gB 07 30 -02.1           ~ 11 0
33 Fermi bn120217808 gB 08 10 +36.8           ~ 12 0
34 Fermi bn130325203 gB 08 11 -18.9           ~ 13 0
35 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
36 Fermi bn120304061 gB 08 29 -61.1           ~ 8 0
37 Fermi bn090804940 gB 08 42 -11.3           ~ 21 0
38 Fermi bn090520876 gB 08 45 -18.0           ~ 13 0
39 Fermi bn110622158 gB 08 56 +19.5           ~ 12 0
40 Fermi bn150220598 gB 09 02 -01.6           ~ 13 0
41 Fermi bn140329295 gB 09 43 -32.2           ~ 17 0
42 Fermi bn140430716 gB 09 46 -36.9           ~ 3 0
43 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
44 Fermi bn110709463 gB 10 22 +23.1           ~ 11 0
45 Fermi bn110903009 gB 10 57 +42.1           ~ 13 0
46 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
47 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
48 GRB 080906B gB 12 11.2 -06 24           ~ 25 0
49 Fermi bn111009282 gB 12 12 -56.8           ~ 10 0
50 Fermi bn140311618 gB 12 14 +62.8           ~ 8 0
51 GRB 131214A gB 12 16 -06.3           ~ 4 0
52 Fermi bn130828808 gB 12 33 +27.9           ~ 3 0
53 GRB 081224A gB 13 26.8 +75 06           ~ 32 0
54 Fermi bn110920338 gB 13 59 -27.6           ~ 28 0
55 Fermi bn140102887 gB 14 07 40.65 +01 19 59.8           ~ 53 0
56 GRB 120919A gB 14 19.1 -45 34           ~ 18 0
57 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 47 0
58 Fermi bn120402669 gB 14 55 -10.4           ~ 12 0
59 GRB 120427A gB 15 00 +29.3           ~ 15 0
60 GRB 120328B gB 15 12 +22.8           ~ 24 0
61 GRB 090620 gB 15 49.4 +61 09           ~ 29 0
62 Fermi bn150118409 gB 16 01 -35.8           ~ 18 0
63 Fermi bn130612456 gB 16 32 +31.0           ~ 6 0
64 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
65 Fermi bn130206482 gB 17 56 +49.4           ~ 4 0
66 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
67 Fermi bn120102095 gB 18 24 53.89 +24 42 47.1           ~ 42 0
68 Fermi bn101208498 gB 18 44 -59.0           ~ 15 0
69 Fermi bn101216721 gB 18 57 -21.0           ~ 16 0
70 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
71 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
72 Fermi bn120222119 gB 19 58 +26.5           ~ 16 0
73 GRB 100528A gB 20 44 29 +27 48.6           ~ 37 0
74 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 116 0
75 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
76 Fermi bn090524346 gB 21 58 -67.4           ~ 20 0
77 GRB 110721A gB 22 10 -38.6           ~ 155 0
78 Fermi bn150721242 gB 22 16 33.6 +07 45 36           ~ 4 0
79 GRB 110318A gB 22 32 -17.8           ~ 28 0
80 GRB 090719 gB 22 45 -67.9           ~ 41 0
81 Fermi bn100707032 gB 23 24 -06.6           ~ 44 0
82 GRB 100612B gB 23 28 -01.8           ~ 23 0
83 GRB 090131 gB 23 29.2 +21 12           ~ 37 0
84 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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