Fig. D.2.

CR proton flux Φp is plotted as a function of kinetic energy Ek. The long dashed-dotted and solid black curves stand respectively for the approximations u0 and uloss. The exact solution u is derived numerically assuming boundary conditions L3 and H4. The long dashed orange and short dashed purple curves correspond to different methods used to solve transport Eq. (4). Protons are injected with a rate where Np = 5.8 × 10−11 protons cm−3 GeV−1 Myr−1 and α = 2.3. With these values, we get Φp in rough agreement with the Voyager 1 (Stone et al. 2013), PAMELA (Adriani et al. 2011) and AMS-02 (Aguilar et al. 2015a) data.
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