Simulations of storm time diffuse aurora with plasmasheet electrons in strong pitch angle diffusion

Using a guiding-center simulation of plasmasheet electrons postulated to be in strong pitch angle diffusion, we compute drift trajectories from a Hamiltonian formulation and map phase space densities from the nightside neutral line in Dungey's model magnetosphere (dipole field plus uniform southward Bz) according to Liouville's theorem modified for exponential loss implicit in the strong diffusion hypothesis. From the resulting phase space distributions we compute the precipitating energy flux into the auroral ionosphere as functions of magnetic latitude and magnetic local time (MLT) so as to simulate numerically the spatial and spectral structure of diffuse auroral electron precipitation for comparison with observational data. Storm-associated impulses (by which we enhance the convection electric field) can typically transport plasmasheet electrons from the nightside neutral line to the near-midnight region of maximum precipitating energy flux (latitude ≈ 65°) in ∼20–30 min, which is roughly the strong diffusion lifetime of 4-keV electrons at the corresponding L value (≈5.7). The maximum precipitating electron energy flux in our simulation of the model storm is thus modulated by random variations in the mean cross-magnetospheric electric potential drop over the 20–30 min before the time of interest. Our results also show a consistent lack of precipitating electron energy flux in the afternoon quadrant, essentially because this is the last quadrant to be visited by plasmasheet electrons (and therefore features the most strongly attenuated phase space densities) as they drift through the magnetosphere on open trajectories. The result agrees qualitatively with the typically observed “darkness” of X-ray images of the diffuse aurora in that sector (1200–1800 MLT). While our simulation results locate the region of maximum energy flux slightly postmidnight during both prestorm and stormtime, in good agreement with previously published statistical compilations of auroral electron precipitation. Our simulations do not explain other large intensifications of electron precipitation (near dawn and in the morning sector) that are also found in both statistical and storm event studies. This suggests the need for a model in which pitch angle diffusion is less than everywhere strong throughout the plasma sheet.

[1]  P. Anderson,et al.  Global storm time auroral X‐ray morphology and timing and comparison with UV measurements , 2000 .

[2]  R. Horne,et al.  The temporal evolution of electron distributions and associated wave activity following substorm injections in the inner magnetosphere , 2000 .

[3]  R. Horne,et al.  Electron pitch angle diffusion by electrostatic electron cyclotron harmonic waves: The origin of pancake distributions , 2000 .

[4]  J. Borovsky,et al.  Plasma sheet access to geosynchronous orbit , 1999 .

[5]  R. Horne,et al.  “Pancake” electron distributions in the outer radiation belts , 1999 .

[6]  S. Cummer,et al.  Global-scale electron precipitation features seen in UV and X rays during substorms , 1999 .

[7]  S. Petrinec,et al.  The position of the auroral energetic electron precipitation region obtained from PIXIE global X-ray observations , 1999 .

[8]  Margaret W. Chen,et al.  Phase-space density mappings for diffuse auroral electrons under strong pitch-angle diffusion in Dungey's model magnetosphere , 1999 .

[9]  P. Anderson,et al.  Energetic auroral electron distributions derived from global X‐ray measurements and comparison with in‐situ particle measurements , 1998 .

[10]  M. Schulz Particle drift and loss rates under strong pitch angle diffusion in Dungey's model magnetosphere , 1998 .

[11]  S. Petrinec,et al.  Statistical Survey of Auroral X-Ray Emissions - Pixie Observations , 1998 .

[12]  B. Anderson,et al.  Onset of nonadiabatic particle motion in the near‐Earth magnetotail , 1997 .

[13]  A. Johnstone Pitch angle diffusion of low energy electrons and positive ions in the inner magnetosphere: A review of observations and theory , 1996 .

[14]  W. J. Burke,et al.  Pitch angle scattering of diffuse auroral electrons by whistler mode waves , 1995 .

[15]  Margaret W. Chen,et al.  Simulations of phase space distributions of storm time proton ring current , 1994 .

[16]  T. L. Schumaker,et al.  Atmospheric energy input and ionization by energetic electrons during the geomagnetic storm of 8–9 November 1991 , 1993 .

[17]  A. Johnstone,et al.  PITCH ANGLE DIFFUSION OF LOW-ENERGY ELECTRONS BY WHISTLER MODE WAVES , 1993 .

[18]  Margaret W. Chen,et al.  Stormtime transport of ring current and radiation belt ions , 1993 .

[19]  Arthur D. Richmond,et al.  Assimilative mapping of ionospheric electrodynamics , 1992 .

[20]  A. R. Kranz,et al.  Heavy ion induced mutations in genetic effective cells of a higher plant. , 1992, Advances in space research : the official journal of the Committee on Space Research.

[21]  M. Schulz,et al.  2 – The Magnetosphere , 1991 .

[22]  H. Koons,et al.  A survey of equatorial magnetospheric wave activity between 5 and 8 RE , 1990 .

[23]  Can Huang,et al.  Spectral characteristics of plasma sheet ion and electron populations during undisturbed geomagnetic conditions , 1989 .

[24]  T. L. Schumaker,et al.  The relationship between diffuse auroral and plasma sheet electron distributions near local midnight , 1989 .

[25]  H. Koons,et al.  A survey of electron cyclotron waves in the magnetosphere and the diffuse auroral electron precipitation , 1989 .

[26]  M. S. Gussenhoven,et al.  A statistical model of auroral ion precipitation , 1989 .

[27]  Arthur D. Richmond,et al.  Mapping electrodynamic features of the high-latitude ionosphere from localized observations: technique , 1988 .

[28]  R. M. Robinson,et al.  On calculating ionospheric conductances from the flux and energy of precipitating electrons , 1987 .

[29]  M. S. Gussenhoven,et al.  A statistical model of auroral electron precipitation , 1985 .

[30]  A. Korth,et al.  Experimental study of the relationship between energetic electrons and ELF waves observed on board GEOS: A support to quasi‐linear theory , 1985 .

[31]  T. Birmingham Pitch angle diffusion in the Jovian magnetodisc , 1984 .

[32]  A. Viñas,et al.  The inner edge of the plasma sheet and the diffuse aurora , 1984 .

[33]  Gérard Belmont,et al.  Are equatorial electron cyclotron waves responsible for diffuse auroral electron precipitation , 1983 .

[34]  M. Blanc,et al.  A theoretical approach to the morphology and the dynamics of diffuse auroral zones , 1983 .

[35]  R. W. Spiro,et al.  Computer simulation of inner magnetospheric dynamics for the magnetic storm of July 29, 1977 , 1982 .

[36]  M. Ashour‐Abdalla,et al.  Electrostatic waves and the strong diffusion of magnetospheric electrons , 1982 .

[37]  R. W. Spiro,et al.  Quantitative simulation of a magnetospheric substorm 1. Model logic and overview , 1981 .

[38]  B. Mauk,et al.  ELECTRON PRECIPITATION OF EVENING DIFFUSE AURORA AND ITS CONJUGATE ELECTRON FLUXES NEAR THE MAGNETOSPHERIC EQUATOR C.-I. Meng Space Sciences Laboratory, University of California, Berkeley, California 94720 , 1979 .

[39]  M. Gough,et al.  Interaction of electrostatic waves with warm electrons at the geomagnetic equator , 1979, Nature.

[40]  G. S. Stiles,et al.  Plasma sheet pressure anisotropies , 1978 .

[41]  M. Ashour‐Abdalla,et al.  Diffuse auroral precipitation. , 1978 .

[42]  D. Southwood The role of hot plasma in magnetospheric convection , 1977 .

[43]  C. Anger,et al.  EMISSIONS BY THE ISIS 2 SATELLITE IN THE 19-24 MLT SECTOR , 1977 .

[44]  M. Schulz Particle lifetimes in strong diffusion , 1974 .

[45]  H. Volland Models of global electric fields within the magnetosphere , 1974 .

[46]  L. Lyons Electron diffusion driven by magnetospheric electrostatic waves , 1974 .

[47]  R. Hoffman,et al.  Electron precipitation patterns and substorm morphology , 1973 .

[48]  C. Kennel,et al.  Satellite studies of magnetospheric substorms on August 15, 1968: 8. Ogo 5 plasma wave observations , 1973 .

[49]  H. Volland A semiempirical model of large‐scale magnetospheric electric fields , 1973 .

[50]  J. H. Mcgehee,et al.  VLF electric field observations in the magnetosphere , 1970 .

[51]  N. Brice Bulk motion of the magnetosphere , 1967 .

[52]  T. R. Hartz,et al.  The general pattern of auroral particle precipitation , 1967 .

[53]  A. Nishida Formation of plasmapause, or magnetospheric plasma knee, by the combined action of magnetospheric convection and plasma escape from the tail , 1966 .

[54]  M. Rosenbluth,et al.  Stability of plasmas confined by magnetic fields , 1957 .