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Energetic electrons in the magnetosphere of Saturn
Author(s) -
Randall B. A.
Publication year - 1994
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/94ja00254
Subject(s) - physics , magnetosphere , saturn , pitch angle , electron , van allen radiation belt , ring current , atomic physics , rings of saturn , enceladus , phase space , plasmasphere , radius , computational physics , astrophysics , nuclear physics , planet , plasma , astronomy , computer security , computer science , thermodynamics
The energy spectra and angular distributions of electrons observed by Pioneer 11 as a function of radial distance in the inner magnetosphere of Saturn are reanalyzed and phase space densities are then calculated. The radial dependence of phase space density requires a distributed loss process. The loss is greatest in the region of the E ring (5.5 < L < 8.5) and is attributed to collisions with the ring particles in agreement with earlier work by Van Allen et al. (1980b). Quantitative analysis yields the following properties of the E ring: the particle radii are in the range of 4 × 10 −5 to 3.2 × 10 −4 cm and the thickness of the ring is approximately 3 R s . Between the inner edge of the E ring (5.5 R s ) and the outer edge of the A ring (2.3 R s ) there are more energetic electrons than can be supplied by radial diffusion from an external source. Detailed calculations show that a cosmic ray albedo neutron decay (CRAND) source in the A and B rings is a plausible source for this excess. The radial diffusion coefficient required to explain the E ring absorption and CRAND source for electrons is 1 × 10 −12 > D 0 > 3 × 10 −12 R s ²/s, assuming that D LL = D 0 L ³. As part of the reanalysis program, a method for the deconvolution of pitch angle distributions observed by simple detectors on a rotating spacecraft is developed. This process removes the instrumental response and rotational smear due to finite sampling periods and yields true angular distributions.

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