2003AJ....125.2291H


Query : 2003AJ....125.2291H

2003AJ....125.2291H - Astron. J., 125, 2291-2298 (2003/May-0)

Optical photometry of GRB 021004: the first month.

HOLLAND S.T., WEIDINGER M., FYNBO J.P.U., GOROSABEL J., HJORTH J., PEDERSEN K., ALVAREZ J.M., AUGUSTEIJN T., CASTRO CERON J.M., CASTRO-TIRADO A., DAHLE H., EGHOLM M.P., JAKOBSSON P., JENSEN B.L., LEVAN A., MOLLER P., PEDERSEN H., PURSIMO T., RUIZ-LAPUENTE P. and THOMSEN B.

Abstract (from CDS):

We present UBVRCICphotometry of the optical afterglow of the gamma-ray burst GRB 021004 taken at the Nordic Optical Telescope between approximately 8 hours and 30 days after the burst. These data are combined with an analysis of the 87 ks Chandra X-ray observations of GRB 021004 taken at a mean epoch of 33 hr after the burst to investigate the nature of this GRB. We find an intrinsic spectral slope at optical wavelengths of β_UH_=0.39±0.12 and an X-ray slope of βX=0.94±0.03. There is no evidence for color evolution between 8.5 hr and 5.5 days after the burst. The optical decay becomes steeper approximately 5 days after the burst. This appears to be a gradual break due to the onset of sideways expansion in a collimated outflow. Our data suggest that the extragalactic extinction along the line of sight to the burst is between AV~0.3 and 0.5 and has an extinction law similar to that of the Small Magellanic Cloud. The optical and X-ray data are consistent with a relativistic fireball with the shocked electrons being in the slow cooling regime and having an electron index of p=1.9±0.1. The burst occurred in an ambient medium that is homogeneous on scales larger than approximately 1018 cm but inhomogeneous on smaller scales. The mean particle density is similar to what is seen for other bursts (0.1 cm–3≲n≲100 cm–3). Our results support the idea that the brightening seen at approximately 0.1 days was due to interaction with a clumpy ambient medium within 1017-1018 cm of the progenitor. The agreement between the predicted optical decay and that observed approximately 10 minutes after the burst suggests that the physical mechanism controlling the observed flux at t~10 minutes is the same as the one operating at t>0.5 days.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays

Nomenclature: Fig.1, Table 1: [HWF2003] A (Nos A-G).

Simbad objects: 15

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Number of rows : 15
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 [HWF2003] E * 00 26 51.42 +18 54 36.0   18.091 17.493     ~ 1 0
2 2MASS J00265236+1856396 * 00 26 52.3638303240 +18 56 39.446126880   19.765 18.287     ~ 1 0
3 [HWF2003] C * 00 26 53.61 +18 56 22.6   21.116 19.741     ~ 1 0
4 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
5 2MASS J00265790+1856067 * 00 26 57.8934718488 +18 56 06.765540684   17.341 16.699     ~ 1 0
6 [HWF2003] F * 00 26 58.77 +18 56 56.0   17.430 16.258     ~ 1 0
7 2MASS J00270054+1854151 * 00 27 00.5564660472 +18 54 14.631228684   17.836 17.323     ~ 1 0
8 2MASS J00270083+1856386 * 00 27 00.8383985280 +18 56 38.461455708   19.480 17.989     ~ 1 0
9 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
10 SN 1978K SN* 03 17 38.620 -66 33 03.40   13.0       SNII 214 1
11 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
12 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
13 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
14 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
15 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2

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