2015ApJ...806..194T


Query : 2015ApJ...806..194T

2015ApJ...806..194T - Astrophys. J., 806, 194 (2015/June-3)

Measuring the bulk Lorentz factors of gamma-ray bursts with Fermi.

TANG Q.-W., PENG F.-K., WANG X.-Y. and TAM P.-H.T.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are powered by ultrarelativistic jets. Usually a minimum value of the Lorentz factor of the relativistic bulk motion is obtained based on the argument that the observed high-energy photons (≫ MeV) can escape without suffering from absorption due to pair production. The exact value, rather than a lower limit, of the Lorentz factor can be obtained if the spectral cutoff due to such absorption is detected. With the good spectral coverage of the Large Area Telescope (LAT) on Fermi, measurements of such a cutoff become possible, and two cases (GRB 090926A and GRB 100724B) have been reported to have high-energy cutoffs or breaks. We systematically search for such high-energy spectral cutoffs/breaks from the LAT and the Gamma-ray Burst Monitor (GBM) observations of the prompt emission of GRBs detected since 2011 August. Six more GRBs are found to have cutoff-like spectral features at energies of ∼10-500 MeV. Assuming that these cutoffs are caused by pair-production absorption within the source, the bulk Lorentz factors of these GRBs are obtained. We further find that the Lorentz factors are correlated with the isotropic gamma-ray luminosity of the bursts, indicating that more powerful GRB jets move faster.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - methods: data analysis - 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 - 2026
#notes
1 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
2 Fermi bn140110263 gB 01 54 20.35 -36 29 44.1           ~ 17 0
3 Fermi bn120316008 gB 03 48 -56.3           ~ 17 0
4 GRB 130502B gB 04 27 02.90 +71 03 38.5           ~ 31 0
5 Fermi bn120830297 gB 05 54 36.0 -28 59 04           ~ 22 0
6 Fermi bn100728095 gB 05 55 02.00 -15 15 20.2           ~ 157 0
7 Fermi bn130504978 gB 06 06 31.29 +03 50 02.0           ~ 27 0
8 Fermi bn131014215 gB 06 41 12.80 -19 05 49.6           ~ 50 0
9 Fermi bn110328520 gB 07 51 +43.1           ~ 17 0
10 GRB 140619B gB 08 51 -09.7           ~ 33 0
11 GRB 140523A gB 08 52 26.70 +24 57 25.6           ~ 24 0
12 Fermi bn131209547 gB 09 06 -33.2           ~ 14 0
13 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
14 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
15 GRB 140729A gB 12 56 +15.4           ~ 13 0
16 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
17 Fermi bn131029973 gB 13 23 +48.3           ~ 13 0
18 Fermi bn140402007 gB 13 50 23.67 +05 46 28.0           ~ 41 0
19 Fermi bn140723067 gB 14 02.5 -03 44           ~ 14 0
20 Fermi bn140102887 gB 14 07 40.65 +01 19 59.8           ~ 53 0
21 GRB 130327B gB 14 31 30.57 -69 24 15.4           ~ 29 0
22 Fermi bn140104731 gB 14 35 01.02 -09 01 41.5           ~ 14 0
23 Fermi bn120107384 gB 16 26 -69.9           ~ 18 0
24 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
25 GRB 130828A gB 17 19 09.240 +28 13 14.05           ~ 16 0
26 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
27 Fermi bn131018673 gB 20 18 08.86 +23 11 15.3           ~ 14 0
28 GRB 130821A gB 20 56 38.440 -12 02 36.53           ~ 25 0
29 Fermi bn140206275 gB 21 01 -08.5           ~ 28 0
30 Fermi bn120709883 gB 21 14 -50.1           ~ 25 0
31 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
32 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
33 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0
34 Fermi bn140323433 gB 23 47 50.31 -79 54 16.4           ~ 36 0

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