2013ApJ...776...95F


Query : 2013ApJ...776...95F

2013ApJ...776...95F - Astrophys. J., 776, 95 (2013/October-3)

High-energy emission of GRB 130427A: evidence for inverse Compton radiation.

FAN Y.-Z., TAM P.H.T., ZHANG F.-W., LIANG Y.-F., HE H.-N., ZHOU B., YANG R.-Z., JIN Z.-P. and WEI D.-M.

Abstract (from CDS):

A nearby superluminous burst GRB 130427A was simultaneously detected by six γ-ray space telescopes (Swift, the Fermi GLAST Burst Monitor (GBM)/Large Area Telescope, Konus-Wind, SPI-ACS/INTEGRAL, AGILE, and RHESSI) and by three RAPTOR full-sky persistent monitors. The isotropic γ-ray energy release is ∼1054 erg, rendering it the most powerful explosion among gamma-ray bursts (GRBs) with a redshift z ≤ 0.5. The emission above 100 MeV lasted about one day, and four photons are at energies greater than 40 GeV. We show that the count rate of 100 MeV-100 GeV emission may be mainly accounted for by the forward shock synchrotron radiation and the inverse Compton radiation likely dominates at GeV-TeV energies. In particular, an inverse Compton radiation origin is favored for the ~(95.3, 47.3, 41.4, 38.5, 32) GeV photons arriving at t ∼ (243, 256.3, 610.6, 3409.8, 34366.2) s after the trigger of Fermi-GBM. Interestingly, the external inverse Compton scattering of the prompt emission (the second episode, i.e., t ∼ 120-260 s) by the forward-shock-accelerated electrons is expected to produce a few γ-rays at energies above 10 GeV, while five were detected in the same time interval. A possible unified model for the prompt soft γ-ray, optical, and GeV emission of GRB 130427A, GRB 080319B, and GRB 090902B is outlined. Implications of the null detection of >1 TeV neutrinos from GRB 130427A by IceCube are discussed.

Abstract Copyright:

Journal keyword(s): gamma rays: general - radiation mechanisms: non-thermal

Simbad objects: 34

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Number of rows : 34
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 3B 940217 gB 01 56.3 +04 33           ~ 204 0
2 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 273 1
3 Fermi bn100206563 gB 03 08 38.94 +13 09 25.5           ~ 126 0
4 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 940 1
5 GRB 071227A gB 03 52 31.09 -55 59 03.3           ~ 175 0
6 GRB 051117B gB 05 40 43.260 -19 16 26.10           ~ 71 0
7 GRB 050826 gB 05 51 01.590 -02 38 35.40           ~ 127 0
8 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 287 1
9 GRB 061006 gB 07 24 07.660 -79 11 55.10           ~ 193 1
10 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 548 0
11 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 163 1
12 GRB 061210 gB 09 38 05.270 +15 37 17.30           ~ 134 0
13 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 145 0
14 GRB 111211A gB 10 12 21.700 +11 12 30.00           ~ 33 0
15 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1209 1
16 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 515 1
17 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 275 1
18 GRB 050509B gB 12 36 18.000 +29 01 24.00           ~ 309 1
19 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 112 1
20 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 467 0
21 GRB 050724 gB 16 24 44.400 -27 32 27.90     19.70     ~ 439 1
22 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 391 0
23 GRB 080905A gB 19 10 39.10 -18 51 55.4           ~ 171 0
24 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1822 2
25 GRB 040701 G 20 47 46.3 -40 14 13           ~ 44 1
26 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 613 1
27 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 259 1
28 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 494 1
29 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 262 1
30 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 234 1
31 GRB 010921 gB 22 55 59.90 +40 55 52.9           ~ 171 1
32 GRB 020819 gB 23 00 12 -43 00.7           ~ 130 1
33 GRB 050709 gB 23 01 26.960 -38 58 39.50           ~ 297 1
34 SN 2012eb SN* 23 41 38.35 -46 11 07.0           SNIb/c 49 1

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