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Effect of the large-scale convection electric field structure on the formation of thin ionization layers at high latitudes
Institution:1. Department of Physics, Indian Institute of Technology Roorkee, Roorkee 247667, Uttarakhand, India;2. National Atmospheric Research Laboratory, Gadanki, India;3. Astronomy Department, Boston University, 725 Commonwealth Avenue, Boston, MA 02215, USA;1. Departamento de Geología, Universidad de Atacama, Av. Copayapu 485, Copiapó, Chile;2. Department of Physics and Geology, University of Perugia, Piazza dell''Università, 06123 Perugia, Italy;3. School of Earth, Atmospheric and Environmental Sciences, University of Manchester, M13 9PL Oxford Road, Manchester, United Kingdom;4. Laboratorio de Análisis por Activación Neutrónica, Centro Atómico de Bariloche, CNEA, Av. Bustillo km 9.5, 8400 Bariloche, Argentina;5. Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Argentina;6. Laboratorio de Estudio y Seguimiento de Volcanes Activos (LESVA), Universidad Nacional de Río Negro, Roca 1242, (8332), Roca, Argentina;7. INENCO/GEONORTE Univ. Nacional de Salta-CONICET, Av. Bolivia 5150-4400, Salta, Argentina;1. School of Chemistry, University of Bristol, BS8 1TS United Kingdom;2. Université de Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumière Matière, Villeurbanne F-69622, France;3. Department of Physics and Centre for Laser, Atomic and Molecular Sciences, University of New Brunswick, Fredericton, NB, Canada;1. Department of Earth and Environmental Sciences, Ludwig-Maximilians-Universität München, Theresienstrasse 41, 80333 Munich, Germany;2. Department of Geological Sciences, The University of Alabama, Box 870338, Tuscaloosa, AL 35404, USA
Abstract:A three-dimensional simulation of the high-latitude ionosphere was applied to investigate the geographical distribution of E-region thin ionization layers which may be formed by the action of the convection electric field. The simulation model computes the ion densities (O+, O+2, N+, N+2, NO+, Fe+), and temperatures as a function of altitude, latitude, and longitude. The stationary state momentum and continuity equations are solved for each ion species, then the energy equation is solved for electrons, neutrals, and a generic ion having the mean ion mass and velocity. The various electric field patterns of the Heppner and Maynard (1987) J. geophys. Res.92, 4467–4489] convection electric field model were applied and the ionization density pattern was examined after a time sufficient for the formation of thin layers (≈2000 s). It was found that large areas of thin ionization layers were formed for each of the electric field patterns examined. Southward IMF Bz conditions resulted in thin layers forming in the pre-midnight sector in the latitude range north of about 70° to about 80°, and after midnight between 60 and 70°. For northward Bz conditions, the layers were mainly in the pre-midnight sector and covered a latitude range from about 60 to 80°.
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