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A REVERSE SHOCK in GRB 160509A
Authors
Alexei V. Filippenko
Andreja Gomboc
+57 more
Atwood W. B.
Carole Mundell
Cenko S. B.
Cenko S. B.
Cenko S. B.
Chevalier R. A.
De Colle F.
Diolaiti E.
Drejc Kopač
Edo Berger
Evans P. A.
Fenimore E. E.
Foreman-Mackey D.
Galama T. J.
Gomboc A.
Gordon K. D.
Granot J.
Harrison R.
Isaac Shivvers
Izzo L.
Japelj J.
Karl M. Menten
Kate D. Alexander
Kennea J. A.
Kennea J. A.
Kobayashi S.
Kobayashi S.
Kopac D.
Laskar T.
Laskar T.
Levan A. J.
Longo F.
MacFadyen A. I.
Melissa L. Graham
Mundell C. G.
Nousek J. A.
Oke J. B.
Panaitescu A.
Perley D. A.
Peter K. G. Williams
Predehl P.
Raffaella Margutti
Rhoads J. E.
Roberts O. J.
Sari R.
Sari R.
Sari R.
Sari R.
Shiho Kobayashi
Stratta G.
Tanmoy Laskar
Tanvir N. R.
WeiKang Zheng
Welty D. E.
Wen-fai Fong
Yost S. A.
Zauderer B. A.
Publication date
28 June 2016
Publisher
'American Astronomical Society'
Doi
View
on
arXiv
Abstract
We present the second multi-frequency radio detection of a reverse shock in a γ-ray burst. By combining our extensive radio observations of the Fermi-Large Area Telescope γ-ray burst 160509A at z = 1.17 up to 20 days after the burst with Swift X-ray observations and ground-based optical and near-infrared data, we show that the afterglow emission comprises distinct reverse shock and forward shock contributions: the reverse shock emission dominates in the radio band at ≲10 days, while the forward shock emission dominates in the X-ray, optical, and near-infrared bands. Through multi-wavelength modeling, we determine a circumburst density of , supporting our previous suggestion that a low-density circumburst environment is conducive to the production of long-lasting reverse shock radiation in the radio band. We infer the presence of a large excess X-ray absorption column, N H ≈ 1.5 ×1022 , and a high rest-frame optical extinction, A V ≈ 3.4 mag. We identify a jet break in the X-ray light curve at , and thus derive a jet opening angle of , yielding a beaming-corrected kinetic energy and radiated γ-ray energy of erg and erg (1-104 keV, rest frame), respectively. Consistency arguments connecting the forward shocks and reverse shocks suggest a deceleration time of s ≈ T 90, a Lorentz factor of , and a reverse-shock-to-forward-shock fractional magnetic energy density ratio of . Our study highlights the power of rapid-response radio observations in the study of the properties and dynamics of γ-ray burst ejecta. © 2016. The American Astronomical Society. All rights reserved
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