Articles | Volume 23, issue 5
Ann. Geophys., 23, 1839–1847, 2005
Ann. Geophys., 23, 1839–1847, 2005

  28 Jul 2005

28 Jul 2005

Proton isotropy boundaries as measured on mid- and low-altitude satellites

N. Yu. Ganushkina1, T. I. Pulkkinen1, M. V. Kubyshkina2, V. A. Sergeev2, E. A. Lvova2, T. A. Yahnina3, A. G. Yahnin3, and T. Fritz4 N. Yu. Ganushkina et al.
  • 1Finnish Meteorological Institute, Space Research Division, FIN-00101 Helsinki, Finland
  • 2Institute of Physics, University of St.-Petersburg, St.-Petersburg, 198904, Russia
  • 3Polar Geophysical Institute, Apatity, Murmansk region, 184200, Russia
  • 4Boston University, Department of Astronomy, Boston, MA 02215, USA

Abstract. Polar CAMMICE MICS proton pitch angle distributions with energies of 31-80 keV were analyzed to determine the locations where anisotropic pitch angle distributions (perpendicular flux dominating) change to isotropic distributions. We compared the positions of these mid-altitude isotropic distribution boundaries (IDB) for different activity conditions with low-altitude isotropic boundaries (IB) observed by NOAA 12. Although the obtained statistical properties of IDBs were quite similar to those of IBs, a small difference in latitudes, most pronounced on the nightside and dayside, was found. We selected several events during which simultaneous observations in the same local time sector were available from Polar at mid-altitudes, and NOAA or DMSP at low-altitudes. Magnetic field mapping using the Tsyganenko T01 model with the observed solar wind input parameters showed that the low- and mid-altitude isotropization boundaries were closely located, which leads us to suggest that the Polar IDB and low-altitude IBs are related. Furthermore, we introduced a procedure to control the difference between the observed and model magnetic field to reduce the large scatter in the mapping. We showed that the isotropic distribution boundary (IDB) lies in the region where Rc/ρ~6, that is at the boundary of the region where the non-adiabatic pitch angle scattering is strong enough. We therefore conclude that the scattering in the large field line curvature regions in the nightside current sheet is the main mechanism producing isotropization for the main portion of proton population in the tail current sheet. This mechanism controls the observed positions of both IB and IDB boundaries. Thus, this tail region can be probed, in its turn, with observations of these isotropy boundaries.

Keywords. Magnetospheric physics (Energetic particles, Precipitating; Magnetospheric configuration and dynamics; Magnetotail)