Generation of energetic proton shells during substorms

The circulation of the terrestrial polar wind during dynamical reconfigurations of the geomagnetic field is systematically examined by means of three-dimensional single-particle codes. In these calculations the storm time collapse of the geomagnetic tail is simulated by a gradual evolution of the Mead and Fairfield (1975) model from disturbed to ground state geometry. The polar wind is considered to consist primarily of protons, distributed throughout the magnetosphere at substorm onset consistently with the large-scale plasma convection. The simulations clearly illustrate the “convection surge” accompanying the development of substorms, displaying an overall earthward compression of the H+ populations. Among these, a dense and low-energy core can be identified at close L shells (within L ∼ 7), which appears as a persistent feature during the dipolarization process. Tailward of these inner regions, the simulations demonstrate a pileup of protons initiated in the mid-tail (∼10–15 RE), which experience intense (several keV) accelerations and pitch angle diffusion owing to the transient breaking of their adiabatic invariants. Most notably, a detailed analysis of the trajectory results reveals a sharp earthward boundary for these newly created energetic H+, which corresponds to the postdipolarization image of the ion adiabatic “threshold” in the geomagnetic tail. Further nonadiabatic considerations suggest that this mechanism which supports the “substorm injection boundary” concept depends upon particle mass per charge and may consequently organize distinct ion layers at the inner edge of the plasma sheet.

[1]  J. Sauvaud,et al.  Dynamics of single‐particle orbits during substorm expansion phase , 1990 .

[2]  S. Krimigis,et al.  The energetic ion substorm injection boundary , 1990 .

[3]  S. Krimigis,et al.  On the relationship between the energetic particle flux morphology and the change in the magnetic field magnitude during substorms , 1989 .

[4]  B. Mauk Generation of macroscopic magnetic-field-aligned electric fields by the convection surge ion acceleration mechanism , 1989 .

[5]  M. Schulz,et al.  Access of energetic particles to storm time ring current through enhanced radial “diffusion” , 1989 .

[6]  T. Moore,et al.  Polar wind ion bands after neutral sheet acceleration , 1989 .

[7]  N. Tsyganenko A magnetospheric magnetic field model with a warped tail current sheet , 1989 .

[8]  C. Meng,et al.  Low altitude observations of dispersionless substorm plasma injections , 1987 .

[9]  C. Meng,et al.  Energy dependence of the equatorward cutoffs in auroral electron and ion precipitation , 1987 .

[10]  S. Krimigis,et al.  Evolution of the ring current during two geomagnetic storms , 1987 .

[11]  G. Gloeckler,et al.  Average spatial distributions of energetic O+, O2+, O6+, and C6+ ions in the magnetosphere observed by AMPTE CCE , 1987 .

[12]  J. Cladis Parallel acceleration and transport of ions from polar ionosphere to plasma sheet , 1986 .

[13]  W. E. Francis,et al.  The polar ionosphere as a source of the storm time ring current , 1985 .

[14]  J. Green,et al.  First measurements of supersonic polar wind in the polar magnetosphere , 1984 .

[15]  B. Mauk,et al.  Dynamical injections as the source of near geostationary quiet time particle spatial boundaries , 1983 .

[16]  R. G. Johnson,et al.  On the Injection Boundary Model and dispersing ion signatures at near-geosynchronous altitudes , 1983 .

[17]  N. Maynard,et al.  Observations of large magnetospheric electric fields during the onset phase of a substorm , 1983 .

[18]  B. Mauk,et al.  Characterization of geostationary particle signatures based on the 'injection boundary' model , 1983 .

[19]  J. Quinn,et al.  Observations of parallel ion energization in the equatorial region , 1982 .

[20]  T. Moore,et al.  Propagating substorm injection fronts , 1981 .

[21]  J. Sauvaud,et al.  Morning sector ion precipitation following substorm injections , 1981 .

[22]  R. Gendrin,et al.  Plasma and Field Signatures of Poleward Propagating Auroral Precipitation Observed at the Foot of the Geos 2 Field Line , 1980 .

[23]  J. Sauvaud,et al.  Dynamics of plasma, energetic particles, and fields near synchronous orbit in the nighttime sector during magnetospheric substorms , 1980 .

[24]  J. Hoffman,et al.  Light ion concentrations and fluxes in the polar regions during magnetically quiet times , 1980 .

[25]  D. Williams,et al.  A source for the geomagnetic storm main phase ring current , 1980 .

[26]  R. Pellinen,et al.  Localized induced electric field within the magnetotail , 1977 .

[27]  D. Williams,et al.  Storm-associated variations of equatorially mirroring ring current protons, 1-800 keV, at constant first adiabatic invariant , 1976 .

[28]  D. Williams,et al.  The storm and poststorm evolution of energetic /35-560 keV/ radiation belt electron distributions , 1975 .

[29]  D. H. Fairfield,et al.  A quantitative magnetospheric model derived from spacecraft magnetometer data , 1975 .

[30]  T. Fritz,et al.  Substorm‐injected protons and electrons and the injection boundary model , 1975 .

[31]  B. Mauk,et al.  Correlation of Kp with the substorm‐injected plasma boundary , 1974 .

[32]  R. Hoffman,et al.  Direct observations in the dusk hours of the characteristics of the storm-time ring current particles during the beginning of magnetic storms , 1974 .

[33]  C. Mcilwain Substorm Injection Boundaries , 1974 .

[34]  E. W. Hones,et al.  Time variations of the magnetotail plasma sheet at 18 RE Determined from concurrent observations by a pair of Vela satellites , 1971 .

[35]  Paul J. Coleman,et al.  Magnetospheric substorms observed at the synchronous orbit. , 1968 .

[36]  F. C. Jones,et al.  Identification of moving magnetic field lines , 1968 .

[37]  T. Northrop Adiabatic charged‐particle motion , 1963 .