Daytime longitudinal structures of electron density and temperature in the topside ionosphere observed by the Hinotori and DEMETER satellites
Author(s) -
Kakinami Y.,
Lin C. H.,
Liu J. Y.,
Kamogawa M.,
Watanabe S.,
Parrot M.
Publication year - 2011
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2010ja015632
Subject(s) - daytime , ionosphere , electron density , electron temperature , f region , atmospheric sciences , geophysics , electron , physics , geology , meteorology , quantum mechanics
Daytime longitudinal structures of the electron density ( N e ) and temperature ( T e ) in the topside ionosphere observed by Hinotori and DEMETER are examined under various conditions of solar flux, local time, and seasons. Results from both satellites show a similar longitudinal N e structure in the morning from July to October, although the value of N e observed by Hinotori is higher than that of DEMETER owing to higher solar flux. This result implies that the longitudinal structure of N e may appear in any solar cycle. Further, a negative correlation between N e and T e in the longitudinal structures appears in the morning when N e is low, while a positive correlation appears around the magnetic equator when N e is sufficiently enhanced during noontime in the high solar flux. A spectrum analysis performed on the DEMETER data reveals that wave numbers 1–2 for N e and T e are dominant and nondominant. The observed wave numbers 3–4 for N e are dominant during November–May and June–October, while they are dominant for T e during October–June and July–September. Both N e and T e show the largest power of wave number 3 in December and wave number 4 in September. Further, observed annual variations of wave numbers 3–4 for N e and T e also differ from wave numbers 3–4 generated by waves in the lower thermosphere. It can be interpreted as discrepancies between the longitudinal distributions of N e and T e caused by difference in the condition of zonal winds driving E region dynamo and meridional winds modulating the ionospheric plasma structures.
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