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  4. A Reverse Shock in GRB 130427A

A Reverse Shock in GRB 130427A

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1305.2453.pdf (373.23 KB)
Date
2013
Author(s)
Laskar, T.
Zauderer, B. A.
Margutti, R.
Chakraborti, S.
Chandra, P.
Ray, A.
DOI
10.1088/0004-637x/776/2/119
Publisher
IOP Publishing
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Citation
Laskar, T., E. Berger, B. A. Zauderer, R. Margutti, A. M. Soderberg, S. Chakraborti, R. Lunnan, R. Chornock, P. Chandra, and A. Ray. 2013. A Reverse Shock in GRB 130427A. The Astrophysical Journal 776, no. 2: 119. doi:10.1088/0004-637x/776/2/119.
Abstract
We present extensive radio and millimeter observations of the unusually bright GRB 130427A at z = 0.340, spanning 0.67 to 12 d after the burst. Taken in conjunction with detailed multi-band UV, optical, NIR, and X-ray observations we find that the broad-band afterglow emission is composed of distinct reverse shock and forward shock contributions. The reverse shock emission dominates in the radio/millimeter and at . 0.1 d in the UV/optical/NIR, while the forward shock emission dominates in the X-rays and at & 0.1 d in the UV/optical/NIR. We further find that the optical and X-ray data require a Wind circumburst environment, pointing to a massive star progenitor. Using the combined forward and reverse shock emission we find that the parameters of the burst are an isotropic kinetic energy of EK,iso ≈ 2×1053 erg, a mass loss rate of M˙ ≈ 3×10−8 M⊙ yr−1 (for a wind velocity of 1,000 km s−1), and a Lorentz factor at the deceleration time of Γ(200s) ≈ 130. Due to the low density and large isotropic energy, the absence of a jet break to ≈ 15 d places only a weak constraint on the opening angle, θj & 2.5◦ , and therefore a total energy of Eγ + EK & 1.2×1051 erg, similar to other GRBs. The reverse shock emission is detectable in this burst due to the low circumburst density, which leads to a slow cooling shock. We speculate that this is a required property for the detectability of reverse shocks in the radio and millimeter bands. Following on GRB 130427A as a benchmark event, observations of future GRBs with the exquisite sensitivity of VLA and ALMA, coupled with detailed modeling of the reverse and forward shock contributions will test this hypothesis.
Other Available Sources
https://arxiv.org/pdf/1305.2453.pdf
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URI
http://nrs.harvard.edu/urn-3:HUL.InstRepos:30485100
Collection
FAS Scholarly Articles
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