2018
DOI: 10.1093/mnras/sty1410
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The effect of cosmic ray acceleration on supernova blast wave dynamics

Abstract: Non-relativistic shocks accelerate ions to highly relativistic energies provided that the orientation of the magnetic field is closely aligned with the shock normal (quasiparallel shock configuration). In contrast, quasi-perpendicular shocks do not efficiently accelerate ions. We model this obliquity-dependent acceleration process in a spherically expanding blast wave setup with the moving-mesh code arepo for different magnetic field morphologies, ranging from homogeneous to turbulent configurations. A Sedov-T… Show more

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Cited by 42 publications
(50 citation statements)
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“…Obliquity-dependency of the acceleration leads to a significant modification of the CR distribution in the shell of the Sedov explosion with either a polar or patchy distribution when the coherence length of the background magnetic field is respectively larger or smaller than the bubble size. This also has consequences on the final shape of the bubble, with a significant elongation of the bubble when the magnetic field has a large field coherence with respect to the bubble size (Pais et al 2018). Finally, the effect of CR streaming and CR acceleration has been tested in an turbulent box mimicking the motions within the interstellar medium on tens of pc scales (Commerçon et al 2019).…”
Section: Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…Obliquity-dependency of the acceleration leads to a significant modification of the CR distribution in the shell of the Sedov explosion with either a polar or patchy distribution when the coherence length of the background magnetic field is respectively larger or smaller than the bubble size. This also has consequences on the final shape of the bubble, with a significant elongation of the bubble when the magnetic field has a large field coherence with respect to the bubble size (Pais et al 2018). Finally, the effect of CR streaming and CR acceleration has been tested in an turbulent box mimicking the motions within the interstellar medium on tens of pc scales (Commerçon et al 2019).…”
Section: Resultsmentioning
confidence: 99%
“…Finally, the new CR energy is updated with ∆e CR = φ CR ∆t/∆x According to detailed simulations of accelerated CRs at shocks (Caprioli & Spitkovsky 2014), their acceleration efficiency depends on both the Mach number of the shock and the upstream magnetic field orientation with respect to the normal to the shock θ B = arccos(b 1 .n s ). The dependency of the efficiency of CR acceleration with this so-called "magnetic obliquity" can be factorized out η(M, X CR , θ B ) = η 0 ξ(M, X CR )ζ(θ B ) and approximated by the following functional form (Pais et al 2018)…”
Section: Cosmic Ray Acceleration At Shocksmentioning
confidence: 99%
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“…Examples include the impact of cosmic rays (e.g. Recchia et al 2016;Pais et al 2018;Jacob et al 2018), stellar jets (Frank et al 2014), high-energy photons from X-ray binaries (Kannan et al 2016b), runaway stars (Kimm & Cen 2014), among others. As such, caution should be exercised when interpreting the results of the models or the meaning of parameters currently used in numerical simulations since they are, by construction, only approximations to the real physics driving the structure and evolution of galaxies.…”
Section: Introductionmentioning
confidence: 99%
“…The degree of sophistication reached by current hydrodynamical simulations is impressive and the level of agreement with observational data encouraging. Recent work has also focused on the inclusion of "non-standard" galaxy formation physics like magnetic fields and cosmic rays (see, e.g., [92,93]). However, different (plausible and often equally successful) physical models for stellar feedback have been proposed (see the discussion in [94]), and it remains difficult to discriminate between them (we will come back to this issue below).…”
Section: Hydrodynamical Simulationsmentioning
confidence: 99%