1993
DOI: 10.1029/93gl02701
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Simulation of the prompt energization and transport of radiation belt particles during the March 24, 1991 SSC

Abstract: We model the rapid (∼ 1 min) formation of a new electron radiation belt at L ≃ 2.5 that resulted from the Storm Sudden Commencement (SSC) of March 24, 1991 as observed by the CRRES satellite. Guided by the observed electric and magnetic fields, we represent the time‐dependent magnetospheric electric field during the SSC by an asymmetric bipolar pulse that is associated with the compression and relaxation of the Earth's magnetic field. We follow the electrons using a relativistic guiding center code. The test‐p… Show more

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Cited by 421 publications
(434 citation statements)
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“…on all (B,L) drift shells. They are energized by time dependent induction electric fields or betatron acceleration, as conclusively demonstrated by the numerical simulations of Li et al (1993). Massive flux enhancements, however, are observed less frequently at the deepest drift shells than at the outermost ones.…”
Section: The Contributions Of the Pioneer And Lunik Missionsmentioning
confidence: 55%
“…on all (B,L) drift shells. They are energized by time dependent induction electric fields or betatron acceleration, as conclusively demonstrated by the numerical simulations of Li et al (1993). Massive flux enhancements, however, are observed less frequently at the deepest drift shells than at the outermost ones.…”
Section: The Contributions Of the Pioneer And Lunik Missionsmentioning
confidence: 55%
“…Specifically, it would be interesting to study the dependence of pitch angle dispersion with ring current intensity and other factors that are parameterized separately in more recent generations of the Tsyganenko models [Tsyganenko, 1995]. For detailed event studies it may be necessary to perform modeling calculations in time-dependent model fields either of MHD model runs or of heuristic models as has recently been done for electrons [Li et al, 1993[Li et al, , 1998]. are correct when the orbits are wrong, the effects of this scattering on the average drift needed to be included in the present calculations.…”
Section: Discussionmentioning
confidence: 99%
“…This indicates that erosion of the plasmapause to low L is one process that occurs simultaneously with electrons being transported to or accelerated at equally low L. It is not clear from the observations in Figure 1 whether the erosion of the plasmapause is a necessary condition for all low-L electron flux enhancements. Shock acceleration of the type that occurred during the famous March 1991 event [Li et al, 1993;Blake et al, 1992] may occur without plasmapause erosion. However, the relationship between plasmapause erosion and low-L electron enhancements needs to be examined in detail.…”
Section: Observationsmentioning
confidence: 99%