Collisional losses of ring current ions

The time evolution of the ring current population during the recovery phase of a typical moderate magnetic storm is studied, using a newly developed kinetic model for H+, He+ and O+ ions which includes nonequatorially mirroring particles. The bounce-averaged distribution function is defined for variables that are accessible to direct measurement, and some useful formulas for calculating the total energy and number density of the ring current are derived. The bounce-averaged kinetic equation is solved, including losses due to charge exchange with neutral hydrogen and Coulomb collisions with thermal plasma along ion drift paths. Time-dependent magnetospheric electric fields and anisotropic initial pitch angle distributions are considered. The generation of ion precipitating fluxes is addressed, a process that is still not completely understood. It is shown that both the decrease of the distribution function due to charge exchange losses and the buildup of a low-energy population caused by Coulomb collisions proceed faster for particles with smaller pitch angles. The maximum of the equatorial precipitating fluxes occurs on the nightside during the early recovery phase and is found to be of the order of 104–105 cm−2sr−1s−1keV−1. The mechanisms considered in this paper indicate that magnetospheric convection plays the predominant role in causing ion precipitation; Coulomb scattering contributes significantly to the low-energy ion precipitation inside the plasmasphere.

[1]  A. J. Chen,et al.  Isolated cold plasma regions - Observations and their relation to possible production mechanisms , 1975 .

[2]  R. LeVeque Numerical methods for conservation laws , 1990 .

[3]  C. E. Rasmussen,et al.  Decay of equatorial ring current ions and associated aeronomical consequences , 1993 .

[4]  D. Stern The motion of a proton in the equatorial magnetosphere , 1975 .

[5]  W. Riedler,et al.  Ring current protons in the upper atmosphere within the plasmasphere , 1976 .

[6]  M. Walt,et al.  Loss cone distributions of radiation belt electrons , 1977 .

[7]  G. Gloeckler,et al.  AMPTE Ion Composition Results , 1987 .

[8]  R. Phaneuf,et al.  Collisions of carbon and oxygen ions with electrons, H, H/sub 2/ and He: Volume 5 , 1987 .

[9]  Ejiri,et al.  Trajectory traces of charged particles in the magnetosphere. [1 to keV] , 1976 .

[10]  Juan G. Roederer,et al.  Dynamics of Geomagnetically Trapped Radiation , 1970 .

[11]  G. Khazanov,et al.  Non-steady-state conditions of filling up the geomagnetic trap with superthermal electrons , 1990 .

[12]  C. Meng,et al.  Substorm introduction of ≤ 1‐keV magnetospheric ions into the inner plasmasphere , 1986 .

[13]  Randall J. LeVeque Conservative Methods for Nonlinear Problems , 1992 .

[14]  Paul G. Richards,et al.  Plasmasphere-ionosphere coupling: 2. Ion composition measurements at plasmaspheric and ionospheric altitudes and comparison with modeling results , 1990 .

[15]  Janet U. Kozyra,et al.  A bounce-averaged kinetic model of the ring current ion population , 1994 .

[16]  C. E. Rasmussen,et al.  A two-dimensional model of the plasmasphere : refilling time constants , 1993 .

[17]  D. V. Sivukhin Motion of Charged Particles in Electromagnetic Fields in the Drift Approximation , 1965 .

[18]  A. Nagy,et al.  The role of ring current O+ in the formation of stable auroral red arcs , 1987 .

[19]  L. Kistler,et al.  Energy spectra of the major ion species in the ring current during geomagnetic storms , 1989 .

[20]  R. Roble,et al.  Observations and theory of the formation of stable auroral red arcs , 1975 .

[21]  E. Parker,et al.  Formation of the geomagnetic storm main‐phase ring current , 1961 .

[22]  R. Sharp,et al.  A comparison of the 0.1-17 keV/e ion composition in the near equatorial magnetosphere between quiet and disturbed conditions , 1982 .

[23]  J. Cornwall,et al.  Observations of precipitating protons in the energy range 2.5 kev≤E≤200 kev , 1971 .

[24]  E. Shelley,et al.  SATELLITE OBSERVATIONS OF ENERGETIC HEAVY IONS DURING A GEOMAGNETIC STORM. , 1972 .

[25]  John D. Craven,et al.  Geocoronal imaging with Dynamics Explorer , 1986 .

[26]  F. Søraas,et al.  Proton observations supporting the ion cyclotron wave heating theory of SAR arc formation , 1978 .

[27]  F. Hinton Collisional transport in plasma , 1983 .

[28]  A. Nagy,et al.  Lifetime of ring current particles due to coulomb collisions in the plasmasphere , 1991 .

[29]  L. Lyons Comments on pitch angle diffusion in the radiation belts , 1973 .

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

[31]  B. M. Reddy,et al.  Global behavior of the ionosphere at 1000‐kilometer altitude , 1967 .

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