Effect of Synchrotron Losses on Multiple Diffusive Shock Acceleration

Abstract The effect of synchrotron losses on diffusive shock acceleration (DSA) at many shocks is treated numerically. Synchrotron losses determine a maximum energy to which electrons can be accelerated through DSA, and this is referred to as the synchrotron cutoff, p c . The distribution of accelerated electrons after many shocks is found (a) for a distribution injected at the initial shock, to tend to a plateau [ f(p) independent of p ≲ 0·1 p c ], and (b) for the cumulative distribution from injection at each shock to tend to f(p) ∝ p –b with b ≈ 3 well below the synchrotron cutoff with a peak in the slope ( b min ≈ 2) at p ≲ 0·1 p c . It is suggested that the latter result might account for the flat synchrotron spectra observed in some Galactic Centre sources.

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