An organized density (and pressure) structure was recently discovered
in the neutral thermosphere at high-latitudes. The structure consists
of two to four high- and low-density regions having diameters of 1000
to 2000 km. The density in each region is enhanced or depleted from th
e hemispheric average by up to 30%. The structure is thus a significan
t feature of the near-Earth space environment at high-latitudes. We re
fer to each distinct region of enhanced or depleted density as a densi
ty ''cell.'' The cells extend upward from about 120 km into the upper
thermosphere, and once formed they remain approximately fixed with res
pect to the geomagnetic pole. A parametric study of the density cell m
orphology for different magnetic activity levels is described for equi
nox solar minimum using the National Center for Atmospheric Research t
hermosphere ionosphere general circulation model (NCAR-TIGCM). Density
data were sought to verify the existence of the structures first pred
icted by the NCAR model. The TIGCM simulations were used to predict th
e large density perturbations observed by the S85-1 satellite in a cir
cular sun-synchronous orbit near 200 km altitudes. The most obvious ma
nifestation of the cells was the presence of density peaks located nea
r 70 degrees Lambda on the dayside and nightside, and a density minimu
m near the magnetic pole. Since high-latitude densities are generally
expected to increase during magnetic activity, the low densities over
the pole are perhaps the most interesting feature of the cell structur
e discussed here. The satellite data confirm the existence of the cell
ular structure over a range of magnetic activity levels. The discovery
of the cells is important because the structure provides a unifying f
ramework for the analysis and interpretation of high-latitude data fro
m both past and future experiments. The cells result from various form
s of coupling between the ionosphere and thermosphere. The cell format
ion is quantitatively consistent with concepts from dynamic meteorolog
y.