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Table 1.
Parameters for two considered scenarios.
Efficient | Test-particle | |
---|---|---|
acceleration | regime | |
Particle | Proton | Eelectron |
diffusion | Bohm | Kolmogorov |
α | 1 | 1/3 |
η | 1 | 10 |
ξcr | 0.15 | – |
Eo | – | 80 GeV |
δB1 | (42) | B1 |
Brad | max(δB1, B1) | B1 |
B1 | 10 μG | 10 μG |
σB |
![]() |
1 |
σtot | 5.5 | 4 |
pmax | min (44), (48) | min (50), (51) |
βa | 9.7 | 20 |
βb | 7.2 | 1 |
Notes. We consider two scenarios for particle acceleration to calculate the evolution of pmax and . We consider two types of particles in order to show the role of the radiative losses in one case and to remove it from analysis in another scenario.
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