2001/04/30 by K. Z. Stanek, Krzysztof Z. Stanek, P. M. Garnavich +12 · 4 citations
Physics and Astronomy · #Astrophysical Phenomena and Observations #Gamma-ray bursts and supernovae #Stellar, planetary, and galactic studies #astro-ph
paper · pdf · doi:10.1086/323941
published as 2001, ApJ, 563, 592 · revised version (minor changes only) to be published in the ApJ Part 1, 12 pages, 4 figures; all data used for the fits and our CCD frames available at ftp://cfa-ftp.harvard.edu/pub/kstanek/GRB010222/ and through WWW at http://cfa-www.harvard.edu/cfa/oir/Research/GRB/
arxiv created 2001/08/10 · openalex publication_date 2001/12/20 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/31
We present the earliest optical observations of the optical counterpart to the gamma-ray burst (GRB) 010222, obtained with the Fred L. Whipple Observatory 1.2 m telescope in UBVRI passbands, starting 3.64 hr after the burst (0.4 hr after public notification of the burst localization). We also present late R -band observations of the afterglow obtained with the 1.8 m Vatican Advanced Technology Telescope ~25 days after the burst. The temporal analysis of our data joined with published data indicates a steepening decay, independent of wavelength, asymptotically approaching F ν ∝ t -0.80±0.05 at early times ( t ≪ 1 day) and F ν ∝ t -1.30±0.05 at late times, with a sharp break at t b = 0.72 ± 0.10 days. This is the second earliest observed break of any afterglow (after GRB 980519), which clearly indicates the importance of rapid multiband follow-up for GRB afterglow research. The optical spectral energy distribution, corrected for small Galactic reddening, can be fitted fairly well by a single power law with F ν ∝ ν -1.07±0.09 . However, when we fit using our BVRI data only, we obtain a shallower slope of -0.88 ± 0.10, in excellent agreement with the slope derived from our low-resolution spectrum (-0.89 ± 0.03). The spectral slope and light-curve decay slopes we derive are not consistent with a jet model despite the presence of a temporal break. Significant host dust extinction with a starburst reddening law would flatten the spectral index to match jet predictions and still be consistent with the observed spectral energy distribution. We derive an opening angle of 2 1, smaller than any listed in the recent compilation of Frail et al. The total beamed energy corrected for the jet geometry is 4 × 10 50 ergs, very close to the "standard" value of 5 × 10 50 ergs found by Frail et al. for a number of other bursts with light-curve breaks.