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Equatorial spread F initiation and growth from satellite traces as revealed from conjugate point observations in Brazil
Author(s) -
Abdu M. A.,
Kherani E. A.,
Batista I. S.,
Reinisch B. W.,
Sobral J. H. A.
Publication year - 2014
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
eISSN - 2169-9402
pISSN - 2169-9380
DOI - 10.1002/2013ja019352
Subject(s) - instability , conjugate , equator , physics , conjugate points , geophysics , geology , atmospheric sciences , geodesy , latitude , mathematics , mechanics , geometry , mathematical analysis
A better understanding of the precursor conditions for the instability growth is very important for identifying the causes of day‐to‐day variability in the equatorial spread F (ESF)/plasma bubble irregularity development. We investigate here the satellite trace (S‐trace) in the ionograms, a precursor to the postsunset ESF occurrence, as observed by Digisondes operated at an equatorial and two magnetic conjugate sites in Brazil during a 66 day observational campaign (Conjugate Point Equatorial Experiment 2002). The satellite traces first occur at the equatorial site, and sequentially, after a variable delay of approximately 20 to 50 min, they are observed nearly simultaneously over the two conjugate sites. The evening prereversal enhancement in the zonal electric field/vertical drift is found to control its development. Using a three‐dimensional simulation code based on collisional interchange instability mechanism, it is shown that the observed S‐trace occurrence sequence is fully consistent with the instability initiation over the equator with the field‐aligned plasma depletion vertical growth marked by latitudinal expansion of its extremities to conjugate locations. The delay in the S‐trace occurrence at the conjugate sites (a measure of the nonlinear growth of the instability for plasma depletion) is controlled also by field line parallel (meridional) neutral wind. The relationship between the S‐trace and the large‐scale wave structure in the F layer, another widely known characterization of the precursor condition for the ESF development, is also clarified.