2010ApJ...725.2209L


Query : 2010ApJ...725.2209L

2010ApJ...725.2209L - Astrophys. J., 725, 2209-2224 (2010/December-3)

Constraining gamma-ray burst initial Lorentz factor with the afterglow onset feature and discovery of a tight Γ0-Eγ,isoCorrelation.

LIANG E.-W., YI S.-X., ZHANG J., LU H.-J., ZHANG B.-B. and ZHANG B.

Abstract (from CDS):

The onset of gamma-ray burst (GRB) afterglow is characterized by a smooth bump in the early afterglow light curve as the GRB fireball is decelerated by the circumburst medium. We extensively search for GRBs with such an onset feature in their optical and X-ray light curves from the literature and from the catalog established with the Swift/XRT. Twenty optically selected GRBs and 12 X-ray-selected GRBs are obtained, among which 17 optically selected and 2 X-ray-selected GRBs have redshift measurements. We fit these light curves with a smooth broken power law and measure the width (w), rising timescale (tr), and decaying timescale (td) at full width at half-maximum. Strong mutual correlations among these timescales and with the peak time (tp) are found. The ratio tr/td is almost universal among bursts, but the ratio tr/tp varies from 0.3 to ∼1. The optical peak luminosity in the R band (LR,p) is anti-correlated with tp and w in the burst frame, indicating a dimmer and broader bump peaking at a later time. The isotropic prompt gamma-ray energy (Eγ,iso) is also tightly correlated with LR,p and tpin the burst frame. Assuming that the bumps signal the deceleration of the GRB fireballs in a constant density medium, we calculate the initial Lorentz factor (Γ0) and the deceleration radius (Rd) of the GRBs with redshift measurements. The derived Γ0 is typically a few hundreds, and the deceleration radius is Rdec∼ 2x1017 cm. More intriguingly, a tight correlation between Γ0 and Eγ,iso is found, namely Γ0≃ 182(Eγ,iso/1052 erg)0.25. This correlation also applies to the small sample of GRBs which show the signature of the afterglow onset in their X-ray afterglow, and to two bursts (GRBs 990123 and 080319B) whose early optical emission is dominated by a reverse shock. The lower limits of Γ0 derived from a sample of optical afterglow light curves showing a decaying feature from the beginning of the observation are also generally consistent with such a correlation. The tight lower limits of Γ0 of GRBs 080916C and 090902B derived from the opacity constraints with Fermi/LAT observations are also consistent with the correlation at the 2σ confidence level, but the short GRB 090510 is a clear outlier of this relation. This correlation may give insight to GRB physics and could serve as an indicator of Γ0 for long GRBs without early afterglow detections. A comparison of the early X-ray and optical afterglow light curves shows that the early bright X-ray emission is usually dominated by a non-forward-shock component, but occasionally (for one case) the forward shock emission is observable, and an achromatic deceleration feature is observed. The superposition of the internal and external components in X-rays causes the diversity of the observed X-ray light curves.

Abstract Copyright: ∼

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

Simbad objects: 51

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Number of rows : 51
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 060912 gB 00 21 08.160 +20 58 17.80 17.61   17.56     ~ 42 0
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
4 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
5 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
6 GRB 070714A gB 02 51 43.36 +30 14 35.1           ~ 63 0
7 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
8 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
9 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
10 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
11 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
12 GRB 080409 gB 05 37 19.20 +05 05 05.1           ~ 38 0
13 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
14 GRB 060804 gB 07 28 49.360 -27 12 56.71 18.74 18.94 17.32     ~ 41 0
15 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
16 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
17 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
18 GRB 080307 gB 09 06 30.73 +35 08 19.8           ~ 53 0
19 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
20 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
21 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
22 GRB 030418 gB 10 54 33.69 -07 01 40.8           ~ 69 0
23 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
24 GRB 060319 gB 11 45 33.050 +60 00 39.61 20.10         ~ 73 0
25 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
26 GRB 090607 gB 12 44 46.70 +44 06 28.4           ~ 40 0
27 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
28 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
29 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
30 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
31 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
32 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
33 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
34 GRB 080507 gB 15 34 43.41 +56 26 08.4           ~ 19 0
35 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
36 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
37 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
38 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
39 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
40 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
41 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
42 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
43 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
44 Fermi bn081126899 gB 21 34 03.54 +48 42 35.2           ~ 76 0
45 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
46 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
47 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
48 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 248 1
49 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
50 GRB 070103 gB 23 30 13.750 +26 52 33.70           ~ 76 0
51 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0

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