Abstract

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.

Highlights

  • The Earth’s radiation belts (ERBs) mainly consist of charged particles with energy from E ∼ 100 keV to several hundreds of megaelectronvolts (MeV)

  • The analysis presented in this paper is limited to the protons of the ERB during magnetically quiet periods of observations (Kp < 2), when the proton fluxes and their spatialenergy distributions were quasi-stationary

  • With respect to the data from the satellites, the pitch angle distributions of the ERB proton fluxes strongly depend on magnetic local time (MLT) at L > 5: the average index A values on the dayside are larger than on the nightside, and this dependence becomes more distinct with increasing energy

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Summary

Introduction

The Earth’s radiation belts (ERBs) mainly consist of charged particles with energy from E ∼ 100 keV to several hundreds of megaelectronvolts (MeV). Compared with the frequencies fc and fb, the drift frequency fd for one particle species has a much narrower range of values; it does not depend on the mass of the particles, and it very weakly depends on the amplitude of their oscillations (∼ 20 % variation). In this case, there are a significant number of particles corresponding to a certain value of fd on each L shell. Kovtyukh: Distribution of Earth’s radiation belts’ protons complete distributions of particles in the ERBs (over the frequency fd) have not been presented nor analyzed; this is the first time.

Constructing the distributions of the ERB protons over their drift frequency
Spatial-energy distributions of the ERB protons near the equatorial plane
Spatial-energy distributions of the ERB protons outside the equatorial plane
Drift frequency distributions of the ERB protons
Findings
Discussion
Conclusions
Full Text
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