On the Structure of Relativistic Collisionless Shocks in Electron-Ion Plasmas
By A. Spitkovsky. 2007
298 citations recorded by the source corpus.
Relativistic collisionless shocks in electron-ion plasmas are thought to occur in the afterglow phase of gamma-ray bursts (GRBs) and in other environments where relativistic flows interact with the interstellar medium. A particular regime of shocks in an unmagnetized plasma has generated much interest for GRB applications. In this Letter, we present ab initio particle-in-cell simulations of unmagnetized relativistic electron-ion shocks. Using long-term 2.5-dimensional simulations with ion-electron mass ratios from 16 to 1000, we resolve the shock formation and reach a steady state shock structure beyond the initial transient. We find that even at high ion-electron mass ratios initially unmagnetized shocks can be effectively mediated by the ion Weibel instability with a typical shock thickness of ~20 ion skin depths. Upstream of the shock, the interaction with merging ion current filaments heats the electron component, so that the postshock flow achieves near-equipartition between the ions and electrons, with the electron temperature reaching 50% of the ion temperature. This energy exchange helps to explain the large electron energy fraction inferred from GRB afterglow observations.
Subfields: Astronomy and Astrophysics, Atomic and Molecular Physics, and Optics
View Paper: https://www.semanticscholar.org/paper/648cc9b7c79f657559f9123c00bf54a1d6944d3f
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Citations in the corpus
- Relativistic Shocks: Particle Acceleration and Magnetization (2015, methodology): “The stream of shock-accelerated particles propagates ahead of the shock, triggering the Weibel instability.”
- FERMI OBSERVATIONS OF GRB 090510: A SHORT–HARD GAMMA-RAY BURST WITH AN ADDITIONAL, HARD POWER-LAW COMPONENT FROM 10 keV TO GeV ENERGIES (2010, background): “Recent particle in cell simulations of relativistic collisionless shocks (Spitkovsky 2008a,b; Martins et al. 2009) suggest that ξe is fairly small (of the order of a few percent), which may in our case allow hνm of several MeV even for low values of ǫB .”
- Nonrelativistic Collisionless Shocks in Unmagnetized Electron-Ion Plasmas (2008, background): “This structure would be formed through the Weibel-type instability like the relativistic shocks in unmagnetized plasmas (Kato 2007; Spitkovsky 2008).”
- PARTICLE ACCELERATION IN RELATIVISTIC MAGNETIZED COLLISIONLESS ELECTRON–ION SHOCKS (2010, background): “…the incoming plasma can filament, and the shock is mediated by the ion Weibel instability (Weibel 1959; Medvedev & Loeb 1999; Gruzinov & Waxman 1999), which ensures strong electron heating and efficient particle acceleration, for both ions and electrons (Spitkovsky 2008a; Martins et al. 2009).”
- Observation of magnetic field generation via the Weibel instability in interpenetrating plasma flows (2013, background): “At time scales longer than those addressed here, this can also lead to the formation of shock waves and to particle acceleration from these shocks [9, 11].”
- Particle Acceleration in Relativistic Collisionless Shocks: Fermi Process at Last? (2008, background): “…Nishikawa et al. 2003, 2005; Silva et al. 2003; Frederiksen et al. 2004; Hededal et al. 2004), and have been evolved through the shock formation stage in both 2D (Gruzinov 2001; Kato 2007; Spitkovsky 2008, hereafter S08; Chang et al. 2008, herefter CSA08) and 3D (Spitkovsky 2005, hereafter S05).”
- The origin of galactic cosmic rays (2013, unknown): “…(PIC) simulations have been instrumental in reaching a better understanding of the formation of collisionless shocks (both relativistic and non-relativistic) and the initial stages of the acceleration process (Spitkovsky 2008a, 2008b; Sironi and Spitkovsky 2011, Gargaté and Spitkovsky 2012).”
- The Binary Neutron Star Event LIGO/Virgo GW170817 160 Days after Merger: Synchrotron Emission across the Electromagnetic Spectrum (2018, result): “These findings are consistent with the picture favored by magnetic field self-generated by the shock is not uniform in the post-shock region, but decays away from the shock (e.g., Spitkovsky 2008; Chang et al. 2008; Keshet et al. 2009; Martins et al. 2009; Haugbølle 2011; Sironi et al. 2013).”
- PARTICLE ACCELERATION IN RELATIVISTIC MAGNETIZED COLLISIONLESS PAIR SHOCKS: DEPENDENCE OF SHOCK ACCELERATION ON MAGNETIC OBLIQUITY (2009, background): “PIC simulations of relativistic unmagnetized shocks have been presented by Spitkovsky (2005, 2008a), Chang et al. (2008) and Keshet et al. (2008); Spitkovsky (2008b) has shown that unmagnetized shocks naturally produce accelerated particles as part of the shock evolution.”
- Reconciling observed gamma-ray burst prompt spectra with synchrotron radiation? (2010, unknown): “More complex distributions showing several components (e.g. Maxwellian distribution+ non-thermal tail) are observed in some simulations of particle acceleration in ultra-relativistic shocks (Spitkovsky 2008b,a; Martins et al. 2009).”
- Relativistic Jets Shine through Shocks or Magnetic Reconnection (2015, methodology): “First-order Fermi acceleration in relativistic shocks has been demonstrated from first principles (Spitkovsky 2008a,b; Martins et al. 2009; Haugbølle 2011; Sironi et al. 2013).”
- THE MAXIMUM ENERGY OF ACCELERATED PARTICLES IN RELATIVISTIC COLLISIONLESS SHOCKS (2013, background): “Shock Structure The physics of electron-ion unmagnetized shocks has been investigated by Spitkovsky (2008a) and Martins et al. (2009) in 2D and by Haugbølle (2011) in 3D.”
- WEIBEL, TWO-STREAM, FILAMENTATION, OBLIQUE, BELL, BUNEMAN...WHICH ONE GROWS FASTER? (2009, background): “For such settings, filamentation instability has been found leading the linear phase, and the shock formation has so far been analyzed accordingly (Medvedev & Loeb 1999; Spitkovsky 2008a, 2008b).”
- ACCELERATION OF PARTICLES AT THE TERMINATION SHOCK OF A RELATIVISTIC STRIPED WIND (2011, background): “Their energization proceeds in the same way as for a strictly unmagnetized shock, which was discussed by Spitkovsky (2008).”