W. Zheng, R. F. Shen, T. Sakamoto, A. P. Beardmore, M. Pasquale, X. F. Wu, J. Gorosabel, Y. Urata, S. Sugita, B. Zhang, A. Pozanenko, M. Nissinen, D. K. Sahu, M. Im, T. N. Ukwatta, M. Andreev, E. Klunko, A. Volnova, C. W. Akerlof, P. Anto, S. D. Barthelmy, A. Breeveld, U. Carsenty, S. Castillo-Carri'on, A. J. Castro-Tirado, M. M. Chester, C. J. Chuang, R. Cunniffe, A. Postigo, R. Duffard, H. Flewelling, N. Gehrels, T. Guver, S. Guziy, V. P. Hentunen, K. Y. Huang, M. Jelínek, T. S. Koch, P. Kub'anek, P. Kuin, T. A. McKay, S. Mottola, S. R. Oates, P. O'Brien, M. J. Page, S. B. Pandey, C. Pulgar, W. Rujopakarn, E. Rykoff, T. Salmi, R. S'anchez-Ramírez, B. E. Schaefer, A. Sergeev, E. Sonbas, A. Sota, J. C. Tello, K. Yamaoka, S. A. Yost, F. Yuan
We present a comprehensive analysis of a bright, long duration (T90 ~ 257 s)
GRB 110205A at redshift z= 2.22. The optical prompt emission was detected by
Swift/UVOT, ROTSE-IIIb and BOOTES telescopes when the GRB was still radiating
in the gamma-ray band. Nearly 200 s of observations were obtained
simultaneously from optical, X-ray to gamma-ray, which makes it one of the
exceptional cases to study the broadband spectral energy distribution across 6
orders of magnitude in energy during the prompt emission phase. By fitting the
time resolved prompt spectra, we clearly identify, for the first time, an
interesting two-break energy spectrum, roughly consistent with the standard GRB
synchrotron emission model in the fast cooling regime. Although the prompt
optical emission is brighter than the extrapolation of the best fit X/gamma-ray
spectra, it traces the gamma-ray light curve shape, suggesting a relation to
the prompt high energy emission. The synchrotron + SSC scenario is disfavored
by the data, but the models invoking a pair of internal shocks or having two
emission regions can interpret the data well. Shortly after prompt emission (~
1100 s), a bright (R = 14.0) optical emission hump with very steep rise (alpha
~ 5.5) was observed which we interpret as the emission from the reverse shock.
It is the first time that the rising phase of a reverse shock component has
been closely observed. The full optical and X-ray afterglow lightcurves can be
interpreted within the standard reverse shock (RS) + forward shock (FS) model.
In general, the high quality prompt emission and afterglow data allow us to
apply the standard fireball shock model to extract valuable information about
the GRB including the radiation mechanism, radius of prompt emission R, initial
Lorentz factor of the outflow, the composition of the ejecta, as well as the
collimation angle and the total energy budget.
View original:
http://arxiv.org/abs/1111.0283
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