2018MNRAS.473.5142C


Query : 2018MNRAS.473.5142C

2018MNRAS.473.5142C - Mon. Not. R. Astron. Soc., 473, 5142-5153 (2018/February-1)

Constraining external reverse shock physics of gamma-ray bursts from ROTSE-III limits.

CUI X.-H., ZOU Y.-C., WEI J.-J., ZHENG W.-K. and WU X.-F.

Abstract (from CDS):

Assuming that early optical emission is dominated by external reverse shock (RS) in the standard model of gamma-ray bursts (GRBs), we intend to constrain RS models with an initial Lorentz factor Γ0 of the outflows based on the ROTSE-III observations. We consider two cases of RS behaviour: relativistic shock and non-relativistic shock. For a homogeneous interstellar medium (ISM) and the wind circum-burst environment, constraints can be achieved by the fact that the peak flux Fν at the RS crossing time should be lower than the observed upper limit F_ν, limit_. We consider the different spectral regimes in which the observed optical frequency νopt may locate, which are divided by the orders for the minimum synchrotron frequency νm and the cooling frequency νc. Considering the homogeneous and wind environments around GRBs, we find that the relativistic RS case can be constrained by the (upper and lower) limits of Γ0 in a large range from about hundreds to thousands for 36 GRBs reported by ROTSE-III. Constraints on the non-relativistic RS case are achieved with limits of Γ0 ranging from ∼30 to ∼350 for 26 bursts. The lower limits of Γ0 achieved for the relativistic RS model are disfavored based on the previously discovered correlation between the initial Lorentz factor Γ0 and the isotropic gamma-ray energy E_γ, iso_ released in the prompt phase.

Abstract Copyright: © 2017 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

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

Simbad objects: 43

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Number of rows : 43
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 091208A gB 00 01 10.90 +65 40 47.7           ~ 24 0
2 Fermi bn100802240 gB 00 09 52.47 +47 45 19.1           ~ 61 0
3 GRB 050922B gB 00 23 13.400 -05 36 17.80           ~ 79 0
4 GRB 070808 gB 00 27 03.40 +01 10 35.4           ~ 55 0
5 Fermi bn090621185 gB 00 43 56.80 +61 56 17.6           ~ 59 0
6 GRB 060312 gB 03 03 05.920 +12 50 02.00           ~ 50 0
7 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
8 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
9 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
10 GRB 050915A gB 05 26 44.804 -28 00 59.27           ~ 88 0
11 GRB 060116 gB 05 38 46.170 -05 26 15.08           ~ 86 0
12 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
13 GRB 080903 gB 05 47 09.60 +51 15 22.4           ~ 38 0
14 GRB 090904A gB 06 43 32.35 +50 12 10.8           ~ 43 0
15 GRB 080303A gB 07 28 14.18 -70 14 03.2           ~ 39 0
16 GRB 071001 gB 09 58 49.7 -59 45 48           ~ 26 0
17 GRB 090715A gB 10 08 24.50 +10 00 22.4           ~ 25 0
18 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
19 GRB 090530 gB 11 57 36.00 +26 35 23.0           ~ 89 0
20 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
21 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
22 GRB 080229 gB 15 12 52.31 -14 42 16.2           ~ 68 0
23 GRB 080604 gB 15 47 51.64 +20 33 28.5           ~ 71 0
24 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
25 GRB 090807 gB 18 14 57.80 +10 16 45.9           ~ 38 0
26 GRB 110315A gB 18 36 46.0 +17 31 56           ~ 28 0
27 GRB 050306 gB 18 49 13.950 -09 09 08.60     19.16     ~ 55 0
28 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
29 GRB 090709A gB 19 19 46.70 +60 43 40.8           ~ 125 0
30 GRB 070429A gB 19 50 48.900 -32 24 17.01           ~ 40 0
31 GRB 071118 gB 19 58 51.77 +70 07 27.9           ~ 44 0
32 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
33 GRB 090727 gB 21 03 50.79 +64 55 29.8           ~ 39 0
34 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
35 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
36 GRB 070621 gB 21 35 10.17 -24 49 02.6           ~ 70 0
37 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
38 GRB 061110A gB 22 25 09.800 -02 15 30.70 21.43         ~ 134 0
39 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
40 GRB 051001 gB 23 23 48.580 -31 31 25.70           ~ 80 0
41 GRB 070704 gB 23 38 47.31 +66 15 12.7           ~ 58 0
42 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0
43 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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