A necessary condition for the formation of thin metallic ion layers in the high-latitude ionosphere, when strong convective electric fields are present, is that these fields have a magnetically westward component. However, observations have shown that proper field direction does not guarantee the occurrence of a layer. A sufficient abundance of metallic ions is also required. We assert that the abundance of metallic ions (and hence occurrence of thin layers) is strongly influenced by large-scale ion transport, which at high latitudes is determined by the spatial and temporal structure of the large-scale convective electric field. A simple model is presented which indicates that on the dayside, ions should be lifted from the nominal background metallic layer below 100 km into the lower F region, where they flow horizontally in a narrow vertical stream (∼50 km) toward the nightside. Upon entering the nightside this stream of metallic ions precipitates within a limited band of geomagnetic latitudes, leading to spatially selective enhancements of ion abundance within the E region. Given an appropriately directed convective electric field, the rate of occurrence of detectable thin ion layers should be greater at those locations where precipitation has occurred and, conversely, should be less where precipitation has not occurred. We suggest that this process controls the abundance of metallic ions and therefore explains the fact that layers are sometimes absent in observations, despite the presence of westwardly directed electric fields.
[1]
J. Grebowsky,et al.
The source of midlatitude metallic ions at F-region altitudes
,
1985
.
[2]
W. Bristow,et al.
Numerical simulation of the formation of thin ionization layers at high latitudes
,
1991
.
[3]
W. B. Hanson,et al.
The morphology of metallic ions in the upper atmosphere
,
1980
.
[4]
D. Krankowsky,et al.
Metal ion layers in the auroral lower E-region measured by mass spectrometers
,
1992
.
[5]
P. Hays,et al.
Theoretical modeling of low‐latitude Mg+
,
1983
.
[6]
T. Nygrén,et al.
The role of electric field and neutral wind direction in the formation of sporadic E-layers
,
1984
.
[7]
U. Zahn,et al.
Formation mechanisms for low‐altitude Es and their relationship with neutral Fe Layers: Results from the METAL Campaign
,
1993
.
[8]
D. Weimer,et al.
Models of high‐latitude electric potentials derived with a least error fit of spherical harmonic coefficients
,
1995
.
[9]
Michael C. Kelley,et al.
The earth's ionosphere
,
1989
.
[10]
U. Zahn,et al.
On the role of auroral electric fields in the formation of low altitude sporadic-E and sudden sodium layers
,
1991
.
[11]
William A. Bristow,et al.
Incoherent scatter observations of thin ionization layers at Sondrestrom
,
1993
.