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Distribution of Earth's radiation belts' protons over the drift frequency of particles
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Abstract. Using data on the proton fluxes of the Earth's radiation belts
(ERBs) with energy ranging from 0.2 to 100 MeV on the drift L shells ranging
from 1 to 8, the quasi-stationary distributions over the drift frequency
fd of protons around the Earth are constructed. For this purpose, direct
measurements of proton fluxes of the ERBs during the period from 1961 to 2017 near the
geomagnetic equator were employed. The main physical processes in the ERB
manifested more clearly in these distributions, and for protons with
fd>0.5 mHz at L>3, their distributions in the {fd,L} space have a more regular shape than
in the {E,L} space. It has also been found that
the quantity of the ERB protons with fd ∼ 1–10 mHz at L∼2
does not decrease, as it does for protons with E > 10–20 MeV (with
fd>10 mHz), but increases with an increase in solar
activity. This means that the balance of radial transport and loss of
ERB low-energy protons at L∼2 is disrupted in favor of transport
of these protons: the effect of an increase in the radial diffusion rates
with increasing solar activity overpowers the effect of an increase in the
density of the dissipative medium.
Title: Distribution of Earth's radiation belts' protons over the drift frequency of particles
Description:
Abstract.
Using data on the proton fluxes of the Earth's radiation belts
(ERBs) with energy ranging from 0.
2 to 100 MeV on the drift L shells ranging
from 1 to 8, the quasi-stationary distributions over the drift frequency
fd of protons around the Earth are constructed.
For this purpose, direct
measurements of proton fluxes of the ERBs during the period from 1961 to 2017 near the
geomagnetic equator were employed.
The main physical processes in the ERB
manifested more clearly in these distributions, and for protons with
fd>0.
5 mHz at L>3, their distributions in the {fd,L} space have a more regular shape than
in the {E,L} space.
It has also been found that
the quantity of the ERB protons with fd ∼ 1–10 mHz at L∼2
does not decrease, as it does for protons with E > 10–20 MeV (with
fd>10 mHz), but increases with an increase in solar
activity.
This means that the balance of radial transport and loss of
ERB low-energy protons at L∼2 is disrupted in favor of transport
of these protons: the effect of an increase in the radial diffusion rates
with increasing solar activity overpowers the effect of an increase in the
density of the dissipative medium.
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