Paz Beniamini
George Washington University
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Publication
Featured researches published by Paz Beniamini.
Monthly Notices of the Royal Astronomical Society | 2015
Paz Beniamini; L. Nava; Rodolfo Barniol Duran; Tsvi Piran
We consider a sample of ten GRBs with long lasting (
Monthly Notices of the Royal Astronomical Society | 2016
Paz Beniamini; Tsvi Piran
\gtrsim10^2\rm\,sec
Monthly Notices of the Royal Astronomical Society | 2014
Paz Beniamini; Tsvi Piran
) emission detected by Fermi/LAT and for which X-ray data around
The Astrophysical Journal | 2016
Paz Beniamini; Kenta Hotokezaka; Tsvi Piran
1\,
Monthly Notices of the Royal Astronomical Society | 2017
Paz Beniamini; Alexander Jonathan Van Der Horst
day are also available. We assume that both the X-rays and the GeV emission are produced by electrons accelerated at the external forward shock, and show that the X-ray and the GeV fluxes lead to very different estimates of the initial kinetic energy of the blast wave. The energy estimated from GeV is on average
Monthly Notices of the Royal Astronomical Society | 2017
Paz Beniamini; Dimitrios Giannios
\sim50
Monthly Notices of the Royal Astronomical Society | 2018
Almog Yalinewich; Paz Beniamini; Kenta Hotokezaka; Wei Zhu
times larger than the one estimated from X-rays. We model the data (accounting also for optical detections around
Monthly Notices of the Royal Astronomical Society | 2018
Paz Beniamini; Dimitrios Giannios; George Younes; Alexander Jonathan Van Der Horst; C. Kouveliotou
1\,
Astronomy and Astrophysics | 2018
Almog Yalinewich; Paz Beniamini
day, if available) to unveil the reason for this discrepancy and find that good modelling within the forward shock model is always possible and leads to two possibilities: either the X-ray emitting electrons (unlike the GeV emitting electrons) are in the slow cooling regime or ii) the X-ray synchrotron flux is strongly suppressed by Compton cooling, whereas, due to the Klein-Nishina suppression, this effect is much smaller at GeV energies. In both cases the X-ray flux is no longer a robust proxy for the blast wave kinetic energy. On average, both cases require weak magnetic fields (
The Astrophysical Journal | 2013
Paz Beniamini; Tsvi Piran
10^{-6}\lesssim \epsilon_B \lesssim 10^{-3}