Two-Dimensional Mapping of Dayside Convection

[1]  Patrick T. Newell,et al.  The cusp and the cleft/boundary layer: Low‐altitude identification and statistical local time variation , 1988 .

[2]  Timothy Fuller-Rowell,et al.  Height-integrated Pedersen and Hall conductivity patterns inferred from the TIROS-NOAA satellite data , 1987 .

[3]  J. Foster,et al.  Plasma convection in the vicinity of the dayside cleft , 1984 .

[4]  R. Heelis.  The effects of interplanetary magnetic field orientation on dayside high‐latitude ionospheric convection , 1984 .

[5]  C. Senior,et al.  MITHRAS: a Brief Description , 1984 .

[6]  J. Evans,et al.  Millstone Hill measurements on 26 February 1979 during the solar eclipse and formation of a midday F-region trough☆ , 1984 .

[7]  J. Foster.  Ionospheric signatures of magnetospheric convection , 1984 .

[8]  R. Heelis,et al.  The relationships between high-latitude convection reversals and the energetic particle morphology observed by Atmosphere Explorer , 1980 .

[9]  K. Verosub,et al.  Is unusual animal behavior observed before earthquakes? Yes and no , 1979 .

[10]  J. Burrows,et al.  Comparison of magnetic field perturbations at high latitudes with charged particle and IMF measurements , 1978 .

[11]  T. Hill,et al.  Solar wind plasma injection at the dayside magnetospheric cusp , 1977 .

[12]  E. W. Hones,et al.  The magnetospheric boundary layer: Site of plasma, momentum and energy transfer from the magnetosheath into the magnetosphere , 1976 .

[13]  V. Wickwar,et al.  Multi-Radar Mapping of Auroral Convection , 1989 .

[14]  J. Foster.  Plasma Transport through the Dayside Cleft: A Source of Ionization Patches in the Polar Cap , 1989 .

[15]  J. V. Evans,et al.  Empirical models for the plasma convection at high latitudes from Millstone Hill observations , 1987 .

[16]  V. Wickwar,et al.  High-Resolution Observations of Electric Fields and F-Region Plasma Parameters in the Cleft Ionosphere , 1985 .

[17]  W. Heikkila.  Definition of the Cusp , 1985 .