Fig. 5

Binned distributions of the exit energies
(red) and the binned contribution of each energy point to the total differential intensity,
(blue), for an initial energy of
MeV. Thereby panel a shows the distribution of exit times of pseudo-particles for a good magnetic connection between the observational point and the Jovian source and panel b for the case of poor magnetic connection. The dashed lines show the integral distribution of the trajectories’ contribution to the total differential intensity as shown in blue.
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