14
Extragalactic and Galactic Cosmic Rays
Authors: Ya. N. Istomin
Number of views: 350
From the analysis of the flux of high energy particles, E > 3·1018eV , it is shown that the
distribution of the power density of extragalactic rays over energy is of the power law, q¯(E) ∝ E
−2.7
,
with the same index of 2.7 that has the distribution of Galactic cosmic rays before so called knee,
E < 3 · 1015eV . However, for the average power of extragalactic sources, which is of E ' 1043erg s−1
,
at least two orders exceeds the power emitted by the Galaxy in cosmic rays, assuming that the
density of galaxies is estimated as Ng ' 1M pc−3
. Considering that such power can be provided by
relativistic jets from active galactic nuclei with the power E ' 1045 − 1046erg s−1
, we estimate the
density of extragalactic sources of cosmic rays as Ng ' 10−2 − 10−3 M pc−3
. Assuming the same
nature of Galactic and extragalactic rays, we conclude that the Galactic rays were produced by a
relativistic jet emitted from the Galactic center during the period of its activity in the past. The
remnants of a bipolar jet are now observed in the form of bubbles of relativistic gas above and
below the Galactic plane. The break, observed in the spectrum of Galactic rays (knee), is explained
by fast escape of energetic particles, E > 3 · 1015eV , from the Galaxy because of the dependence of
the coefficient of diffusion of cosmic rays on energy, D ∝ E
0.7
. The obtained index of the density
distribution of particles over energy, N(E) ∝ E
−2.7−0.7/2 = E
−3.05, for E > 3 · 1015eV agrees well
with the observed one, N(E) ∝ E
−3.1
. Estimated time of termination of the jet in the Galaxy is
4.2 · 104
years ago.