4.6 Article

Physics of the GRB 030328 afterglow and its environment

期刊

ASTRONOMY & ASTROPHYSICS
卷 455, 期 2, 页码 423-U13

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361:20054728

关键词

gamma rays : bursts; radiation mechanisms : non-thermal; line : identification; cosmology : observations

资金

  1. Science and Technology Facilities Council [PP/D000920/1] Funding Source: researchfish
  2. STFC [PP/D000920/1] Funding Source: UKRI

向作者/读者索取更多资源

Aims. To investigate the physical nature of the afterglow emission. We report on the photometric, spectroscopic and polarimetric observations of the optical afterglow of Gamma-Ray Burst (GRB) 030328 detected by HETE-2. Methods. Photometric, spectroscopic and polarimetric monitoring of the optical afterglow. Results. Photometry, collected at 7 different telescopes, shows that a smoothly broken powerlaw decay, with indices alpha(1) = 0.76 +/- 0.03, alpha(2) = 1.50 +/- 0.07 and a break at t(b) = 0.48 +/- 0.03 days after the GRB, provides the best fit of the optical afterglow decline. This shape is interpreted as due to collimated emission, for which we determine a jet opening angle theta(jet) similar to 3 degrees.2. An achromatic bump starting around similar to 0.2 d after the GRB is possibly marginally detected in the optical light curves. Optical spectroscopy shows the presence of two rest-frame ultraviolet metal absorption systems at z = 1.5216 +/- 0.0006 and at z = 1.295 +/- 0.001, the former likely associated with the GRB host galaxy. Analysis of the absorption lines at z = 1.5216 suggests that the host of this GRB may be a Damped Lyman-alpha Absorber. The optical V-band afterglow appears polarized, with P = (2.4 +/- 0.6)% and theta = 170 degrees +/- 7 degrees, suggesting an asymmetric blastwave expansion. An X-ray-to-optical spectral flux distribution of the GRB 030328 afterglow was obtained at 0.78 days after the GRB and fitted using a broken powerlaw, with an optical spectral slope beta(opt) = 0.47 +/- 0.15, and an X-ray slope beta(X) = 1.0 +/- 0.2. Conclusions. The discussion of the results in the context of the fireball model shows that the preferred scenario for this afterglow is collimated structured jet with fixed opening angle in a homogeneous medium.

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