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Cosmic-ray acceleration by forward and reverse shocks in young SNR

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Presentation on theme: "Cosmic-ray acceleration by forward and reverse shocks in young SNR"— Presentation transcript:

1 Cosmic-ray acceleration by forward and reverse shocks in young SNR
Martin Pohl U-Potsdam and DESY Zeuthen with Igor Telezhinsky and Vikram Dwarkadas

2 Modelling methods Gas hydro with semi-analytical acceleration
Gas hydro + CR acceleration and transport Full account of gas, CRs, and MF only plane-parallel shock, no transport can include CR feedback accurate CR transport multiple shocks possible CR feedback difficult maybe at ICRC

3 Hydrodynamical profiles
Often assumed: Sedov phase Late time only!

4 Reality: dynamical evolution
Typically at least 2 shocks! Acceleration everywhere, because

5 The method 1. Use flow profiles from hydrodynamical simulations
2. Solve CR transport equation for these flow profiles. Advantage: Accurate treatment of acceleration and transport Consistent account of escape possible Disadvantage: No account for CR feedback (works for low CR pressure)

6 The method Transformation of spatial coordinate required
Diffusion coefficient can be coupled to MF profile 2 MF profiles used thus far D: density scaling P: pressure scaling 4. Multiple shocks can be accounted for 5. Self-consistent calculation of emission

7 Magnetic-field profiles
Examples of MF profiles for Type 1a Magnetic-field amplification at shocks M1: Caprioli et al. 2009 M2: constant amplification factor More accurate MF transport forthcoming

8 Particle spectra Note the bumps in the spectra! Electrons Protons
Here density scaling of MF with 75 mG at forward shock Note the bumps in the spectra!

9 It is critical to know where gas and MF sits
Emission (Type 1a) It is critical to know where gas and MF sits

10 With more MF amplification
Electrons Protons Again density scaling, but relative to Caprioli model at forward shock

11 Emission (Type 1a)

12 Surface Brightness Maps
M M2 RADIO 1.4GHz SY 3 keV PD 1 TeV IC 1 TeV

13 Conclusions Realistic fluid profiles are important for modeling
Reverse shock can dominate for young SNR Adiabatic cooling/heating throughout the system Complicated particle / emission spectra Hard gamma-ray spectra don‘t always imply CR modification


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