Populating of the cusp and boundary layers by energetic (hundreds of keV) equatorial particles

We examine the dynamics of charged particles in the frontside magnetosphere. We show that the existence of a magnetic field minimum in the outer cusp region has significant implications for the large-scale transport of energetic (a few hundreds of keV) particles that are trapped near the equator. Upon approach (within a few Earth radii) of the magnetopause in the day side sector, these particles are subjected to a mirror force pointing away from the equator and may escape toward high latitudes. We demonstrate that via this process, energetic electrons and ions from the outer radiation belts and ring current may leak into the outer cusp and be scattered back into the nightside plasma sheet. During transport, the particle behavior critically depends upon gradient drift timescale as compared with convection timescale. We show that by diverting energetic equatorial particles toward the frontside magnetopause, dynamical reconfiguration of the magnetospheric field lines during substorms may favor such injections toward high latitudes and loading of the outer cusp. At a given energy, equatorial particles with higher charge state (i.e., larger drift timescale) reside longer in the dayside magnetosphere and are thus more susceptible to transport toward the field minimum.

[1]  J. Sauvaud,et al.  Recirculation of plasma sheet particles into the high‐latitude boundary layer , 1998 .

[2]  T. Mukai,et al.  Statistical properties and possible supply mechanisms of tailward cold O + beams in the lobe/mantle regions , 1998 .

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

[4]  Christopher T. Russell,et al.  Comparison of observed and model magnetic fields at high altitudes above the polar cap: POLAR initial results , 1997 .

[5]  H. Spence,et al.  A new, temporarily confined population in the polar cap during the August 27, 1996 geomagnetic field distortion period , 1997 .

[6]  Yehuda Ben-Zion,et al.  Wrinkle-like slip pulse on a fault between different , 1997 .

[7]  J. Sauvaud,et al.  On the nonadiabatic precipitation of ions from the near-Earth plasma sheet , 1996 .

[8]  A. E. Antonova High-latitude particle traps and related phenomena , 1996 .

[9]  Nikolai A. Tsyganenko,et al.  Modeling the Earth's magnetospheric magnetic field confined within a realistic magnetopause , 1995 .

[10]  T. Onsager,et al.  Model of magnetosheath plasma in the magnetosphere: Cusp and mantle particles at low‐altitudes , 1993 .

[11]  J. Sauvaud,et al.  Nonadiabatic transport features in the outer cusp region , 1992 .

[12]  D. Fairfield Advances in magnetospheric storm and substorm research: 1989–1991 , 1992 .

[13]  M. Allen,et al.  Enhancement of atmospheric radiation by an aerosol layer. , 1992, Journal of geophysical research.

[14]  E. Donovan,et al.  Internal consistency of the Tsyganenko Magnetic Field Model and the Heppner‐Maynard Empirical Model of the ionospheric electric field distribution , 1991 .

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

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

[17]  Mike Lockwood,et al.  Interplanetary magnetic field control of dayside auroral activity and the transfer of momentum across the dayside magnetopause , 1989 .

[18]  Lev M. Zelenyi,et al.  Regular and chaotic charged particle motion in magnetotaillike field reversals: 1. Basic theory of trapped motion , 1989 .

[19]  T. Engelder,et al.  Correction [to “An experimental study of permeability and fluid chemistry in an artificially jointed marble” by Chris Marone, James Rubenstone, and Terry Engelder] , 1989 .

[20]  Nikolai A. Tsyganenko,et al.  GLOBAL QUANTITATIVE MODELS OF THE GEOMAGNETIC-FIELD IN THE CISLUNAR MAGNETOSPHERE FOR DIFFERENT DISTURBANCE LEVELS , 1987 .

[21]  N. Maynard,et al.  Empirical high‐latitude electric field models , 1987 .

[22]  B. Mauk Quantitative modeling of the “convection surge” mechanism of ion acceleration , 1986 .

[23]  E. G. Shelley,et al.  Survey of 0.1- to 16-keV/e plasma sheet ion composition , 1986 .

[24]  V. A. Sergeev,et al.  Pitch-angle scattering of energetic protons in the magnetotail current sheet as the dominant source of their isotropic precipitation into the nightside ionosphere , 1983 .

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

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

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

[28]  L. Friesen,et al.  A simple model of the magnetosphere , 1979 .

[29]  H. Volland A model of the magnetospheric electric convection field , 1978 .

[30]  B. Tsurutani,et al.  Two types of magnetospheric ELF chorus and their substorm dependences , 1977 .

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

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

[33]  A. E. Antonova,et al.  STRUCTURE OF THE GEOMAGNETIC FIELD AT GREAT DISTANCES FROM THE EARTH. , 1968 .

[34]  F. R. Scott,et al.  The Adiabatic Motion of Charged Particles , 1964 .

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

[36]  J. Sauvaud,et al.  Two-point measurement of hot plasma structures in the magnetotail lobes , 1997 .

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

[38]  V. P. Shabansky Some processes in the magnetosphere , 1971 .

[39]  S. Chapman,et al.  A new theory of magnetic storms , 1931 .

[40]  Jiasheng Chen,et al.  University of New Hampshire Scholars' Repository University of New Hampshire Scholars , 2022 .