Projects per year
Abstract
Introduction: In this study, we use 7 years (2012–2019) of pitch angle resolved electron flux measurements from Van Allen Probe-B spacecraft to study the variation of near-equatorial pitch angle distributions (PADs) of outer radiation belt (L <inline-formula id="inf1" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 3) relativistic electrons (E <inline-formula id="inf2" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 0.5 MeV) with different levels of geomagnetic activity.
Methods: We calculate a pitch angle anisotropy index (PAI) to categorize the PADs into three types: pancake, PAI <inline-formula id="inf3" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 1.05; butterfly, PAI <inline-formula id="inf4" style="-webkit-font-smoothing: antialiased;">≤≤</inline-formula> 0.95; and flattop, 0.95 <inline-formula id="inf5" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> PAI <inline-formula id="inf6" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 1.05.
Results and Discussion: Our statistical results show that L shells <inline-formula id="inf7" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 5 are dominated by pancake PADs on the dayside (9 <inline-formula id="inf8" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf9" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 15), butterfly PADs on the nightside (21 <inline-formula id="inf10" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf11" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 3), and flattop PADs in the dawn (3 <inline-formula id="inf12" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf13" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 9) and dusk (15 <inline-formula id="inf14" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf15" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 21) sectors, across almost all relativistic energies. In the inner L shells, the pancake and flattop PADs exhibit dependence on both L-shell and energy, with the occurrence rate increasing with decreasing L and increasing energy. For the butterfly PADs, we discovered a second population of low-L butterflies that are present at almost all local times. When the variation of electron PAI is compared with solar wind dynamic pressure <inline-formula id="inf16" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula> and geomagnetic indices SYM-H and AL, <inline-formula id="inf17" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula> is found to be the dominant parameter in driving the outer radiation belt pitch angle anisotropy. During periods of enhanced <inline-formula id="inf18" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula>, pancake PADs on the dayside become more <inline-formula id="inf19" style="-webkit-font-smoothing: antialiased;">90°90°</inline-formula>-peaked, butterfly PADs on the nightside exhibit enhanced flux dips around <inline-formula id="inf20" style="-webkit-font-smoothing: antialiased;">90°90°</inline-formula> pitch angle along with an enhanced azimuthal and radial extent, and flattop PADs turn into either pancake or butterfly PADs.
Methods: We calculate a pitch angle anisotropy index (PAI) to categorize the PADs into three types: pancake, PAI <inline-formula id="inf3" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 1.05; butterfly, PAI <inline-formula id="inf4" style="-webkit-font-smoothing: antialiased;">≤≤</inline-formula> 0.95; and flattop, 0.95 <inline-formula id="inf5" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> PAI <inline-formula id="inf6" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 1.05.
Results and Discussion: Our statistical results show that L shells <inline-formula id="inf7" style="-webkit-font-smoothing: antialiased;">≥≥</inline-formula> 5 are dominated by pancake PADs on the dayside (9 <inline-formula id="inf8" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf9" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 15), butterfly PADs on the nightside (21 <inline-formula id="inf10" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf11" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 3), and flattop PADs in the dawn (3 <inline-formula id="inf12" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf13" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 9) and dusk (15 <inline-formula id="inf14" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> MLT <inline-formula id="inf15" style="-webkit-font-smoothing: antialiased;"><<</inline-formula> 21) sectors, across almost all relativistic energies. In the inner L shells, the pancake and flattop PADs exhibit dependence on both L-shell and energy, with the occurrence rate increasing with decreasing L and increasing energy. For the butterfly PADs, we discovered a second population of low-L butterflies that are present at almost all local times. When the variation of electron PAI is compared with solar wind dynamic pressure <inline-formula id="inf16" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula> and geomagnetic indices SYM-H and AL, <inline-formula id="inf17" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula> is found to be the dominant parameter in driving the outer radiation belt pitch angle anisotropy. During periods of enhanced <inline-formula id="inf18" style="-webkit-font-smoothing: antialiased;">PdynPdyn</inline-formula>, pancake PADs on the dayside become more <inline-formula id="inf19" style="-webkit-font-smoothing: antialiased;">90°90°</inline-formula>-peaked, butterfly PADs on the nightside exhibit enhanced flux dips around <inline-formula id="inf20" style="-webkit-font-smoothing: antialiased;">90°90°</inline-formula> pitch angle along with an enhanced azimuthal and radial extent, and flattop PADs turn into either pancake or butterfly PADs.
Original language | English |
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Article number | 1474503 |
Pages (from-to) | 1-16 |
Number of pages | 16 |
Journal | Frontiers in Astronomy and Space Sciences |
Volume | 11 |
DOIs | |
Publication status | Published - 19 Dec 2024 |
Keywords
- outer radiation belt
- Relativistic Electrons
- pitch angle distribution
- Pitch angle anisotropy
- Anisotropy index
- Solar wind parameters
- Geomagnetic indices
- Van Allen Probes
Projects
- 1 Active
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STFC Consolidated Grant for the Solar and Space Physics Group at Northumbria University
McLaughlin, J. (PI), Bentley, S. (CoI), Rae, J. (CoI), Jeffrey, N. (CoI), Coxon, J. (CoI) & Watt, C. (CoI)
Science and Technologies Facilities Council
1/04/23 → 31/03/26
Project: Research