Fig. 10

Evolution of loss cone α (red) and pitch angle θ (black) for a simplified CMT acceleration model (model 1) with constant loop top velocity vLT(t). Shown are the results for three different starting pitch angles θi close to the critical initial pitch angle. One can see that both Fermi and Betatron accelerations are operating simultaneously, however, betatron acceleration is the overall dominating mechanism, causing θ to increase.
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