Drift phase resolved diffusive radiation belt model: 1. Theoretical framework

Most physics-based models provide a coarse three-dimensional representation of radiation belt dynamics at low time resolution, of the order of a few drift periods. The description of the effect of trapped particle transport on radiation belt intensity is based on the random phase approximation, and...

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Main Authors: Solène Lejosne, Jay M. Albert
Format: Article
Language:English
Published: Frontiers Media S.A. 2023-07-01
Series:Frontiers in Astronomy and Space Sciences
Subjects:
Online Access:https://www.frontiersin.org/articles/10.3389/fspas.2023.1200485/full
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author Solène Lejosne
Jay M. Albert
author_facet Solène Lejosne
Jay M. Albert
author_sort Solène Lejosne
collection DOAJ
description Most physics-based models provide a coarse three-dimensional representation of radiation belt dynamics at low time resolution, of the order of a few drift periods. The description of the effect of trapped particle transport on radiation belt intensity is based on the random phase approximation, and it is in one dimension only: the third adiabatic invariant coordinate, akin to a phase-averaged radial distance. This means that these radiation belt models do not resolve the drift phase or, equivalently, the magnetic local time. Yet, in situ measurements suggest that radiation belt intensity frequently depends on magnetic local time, at least transiently, such as during active times. To include processes generating azimuthal variations in trapped particle fluxes and to quantify their relative importance in radiation belt energization, an improvement in the spatiotemporal resolution of the radiation belt models is required. The objective of this study is to pave the way for a new generation of diffusive radiation belt models capable of retaining drift phase information. Specifically, we highlight a two-dimensional equation for the effects of trapped particle transport on radiation belt intensity. With a theoretical framework that goes beyond the radial diffusion paradigm, the effects of trapped particle bulk motion, as well as diffusion, are quantified in terms of Euler potentials, α,β, quantities akin to the radial and azimuthal directions. This work provides the theoretical foundations underlying the drift phase resolved transport equation for radiation belt dynamics. It also brings forward the concept of azimuthal diffusion as a phase-mixing agent.
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spelling doaj.art-a4d86453409e4f7b8a5fae641ca45f6b2023-07-04T06:45:41ZengFrontiers Media S.A.Frontiers in Astronomy and Space Sciences2296-987X2023-07-011010.3389/fspas.2023.12004851200485Drift phase resolved diffusive radiation belt model: 1. Theoretical frameworkSolène Lejosne0Jay M. Albert1Space Sciences Laboratory, University of California, Berkeley, Berkeley, CA, United StatesAir Force Research Laboratory, Kirtland AFB, Albuquerque, NM, United StatesMost physics-based models provide a coarse three-dimensional representation of radiation belt dynamics at low time resolution, of the order of a few drift periods. The description of the effect of trapped particle transport on radiation belt intensity is based on the random phase approximation, and it is in one dimension only: the third adiabatic invariant coordinate, akin to a phase-averaged radial distance. This means that these radiation belt models do not resolve the drift phase or, equivalently, the magnetic local time. Yet, in situ measurements suggest that radiation belt intensity frequently depends on magnetic local time, at least transiently, such as during active times. To include processes generating azimuthal variations in trapped particle fluxes and to quantify their relative importance in radiation belt energization, an improvement in the spatiotemporal resolution of the radiation belt models is required. The objective of this study is to pave the way for a new generation of diffusive radiation belt models capable of retaining drift phase information. Specifically, we highlight a two-dimensional equation for the effects of trapped particle transport on radiation belt intensity. With a theoretical framework that goes beyond the radial diffusion paradigm, the effects of trapped particle bulk motion, as well as diffusion, are quantified in terms of Euler potentials, α,β, quantities akin to the radial and azimuthal directions. This work provides the theoretical foundations underlying the drift phase resolved transport equation for radiation belt dynamics. It also brings forward the concept of azimuthal diffusion as a phase-mixing agent.https://www.frontiersin.org/articles/10.3389/fspas.2023.1200485/fullradiation beltsFokker–Planck equationadiabatic invariantsEuler potentialsradial transportradial diffusion
spellingShingle Solène Lejosne
Jay M. Albert
Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
Frontiers in Astronomy and Space Sciences
radiation belts
Fokker–Planck equation
adiabatic invariants
Euler potentials
radial transport
radial diffusion
title Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
title_full Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
title_fullStr Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
title_full_unstemmed Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
title_short Drift phase resolved diffusive radiation belt model: 1. Theoretical framework
title_sort drift phase resolved diffusive radiation belt model 1 theoretical framework
topic radiation belts
Fokker–Planck equation
adiabatic invariants
Euler potentials
radial transport
radial diffusion
url https://www.frontiersin.org/articles/10.3389/fspas.2023.1200485/full
work_keys_str_mv AT solenelejosne driftphaseresolveddiffusiveradiationbeltmodel1theoreticalframework
AT jaymalbert driftphaseresolveddiffusiveradiationbeltmodel1theoreticalframework