2011
DOI: 10.1016/j.crhy.2011.01.011
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Shock acceleration in gamma-ray bursts

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Cited by 5 publications
(2 citation statements)
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“…The fluid description erases all information of the particle momentum distribution. The usual assumption is that the wind particles will be accelerated to a powerlaw distribution in energy, an assumption that is required by observations but remains challenging to prove theoretically (Lemoine & Pelletier 2011). Numerical simulations find this occurs in unmagnetised pair plasmas (Spitkovsky 2008) or for nearly parallel magnetised shocks (Sironi & Spitkovsky 2009).…”
Section: The Transition To High-mass X-ray Binaries: Propellersmentioning
confidence: 99%
“…The fluid description erases all information of the particle momentum distribution. The usual assumption is that the wind particles will be accelerated to a powerlaw distribution in energy, an assumption that is required by observations but remains challenging to prove theoretically (Lemoine & Pelletier 2011). Numerical simulations find this occurs in unmagnetised pair plasmas (Spitkovsky 2008) or for nearly parallel magnetised shocks (Sironi & Spitkovsky 2009).…”
Section: The Transition To High-mass X-ray Binaries: Propellersmentioning
confidence: 99%
“…The instantaneous synchrotron spectrum at a given shock location depends on three physical quantities: the slope p and minimum Lorentz factor γm of the initial distribution of electrons, and the magnetic field strength B. The last two are estimated by assuming that respective fractions ǫe and ǫB of the dissipated energy (in the local fluid frame) are used to accelerate electrons and amplify the magnetic field [9]. Comparing the hydrodynamical expansion time to the synchrotron cooling time then leads to define the Lorentz factor γc: electrons with Lorentz factors γ > γc can radiate efficiently while those with γ < γc mostly loose their energy by adiabatic expansion.…”
Section: Standard Model Of the Afterglowmentioning
confidence: 99%