Abstract
The steady state of cosmic-ray nuclei in interstellar space is discussed. It is shown that for a steady-state situation (or for any mode of propagation in which the allowed path lengths between the source and observer have a wide distribution), the generally used matter-slab approximation for the interstellar matter traversed by cosmic rays leads to erroneous conclusions. The steady-state energy spectra of heavy nuclei are found to have negative slopes down to energies , if the injection spectra are like a rigidity power law; this offers an explanation for the apparently surprising observation of flat spectra for heavy nuclei down to energies . Further it is found that the ratio cannot keep on increasing at low energies but must decrease continuously below a few hundred , even for energy-independent fragmentation cross sections; this also is in accord with recent experimental results.
- Received 13 December 1966
DOI:https://doi.org/10.1103/PhysRev.158.1238
©1967 American Physical Society