Fig. 11.

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Impact of proton–proton losses on the maximum energy. Left: ratio Ėpp/ĖDSA as a function of the proton energy for ρ0. Right: maximum CR energy as limited by proton–proton interactions for a flat density profile with density (ρ0, black) or a steady-wind profile (Eq. (6); red), for different magnetic fields. Emax is derived by imposing ĖDSA =Ėpp at the Bohm limit, and employing the parametrisation from Krakau & Schlickeiser (2015) for the proton–proton losses.
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