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    Equatorial North‐South Difference of Noontime Electron Density Bite‐Out in the F2 Layer
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    Abstract:
    Abstract Noontime bite‐out (depletion) of N m F 2 (peak electron density of the F 2 layer) often occurs in the equatorial ionosphere; it is characterized by a noontime minimum sandwiched by a prenoon peak and a postnoon peak of N m F 2 . The fountain effect was suggested to be responsible for this abnormal diurnal variation pattern. Noontime bite‐out should occur not only at the dip equator but also concurrently at both equatorial north and south according to the fountain effect mechanism. In this study, ionosonde measurements in the equatorial ionization anomaly trough region were selected to investigate the climatology of noontime bite‐out. North‐south difference of noontime bite‐out was presented for the first time. Noontime bite‐out occurs near the dip equator in all months. However, N m F 2 enhances continuously since early morning till late afternoon at equatorial north (south) in northern summer (winter) months; nevertheless, noontime bite‐out still occurs in other months. This cannot be understood only in terms of the fountain effect mechanism. We suggested the reason is seasonally dependent transequator plasma transport induced by neutral meridional winds. Transequator transport works since early morning to modulate N m F 2 variation pattern in daytime. Plasma outflow induced by the transequator transport results in significant N m F 2 depletion at equatorial north or south before the fountain effect induced bite‐out; thus, N m F 2 prenoon peak is restrained and noontime bite‐out variation pattern is absent.
    Keywords:
    Ionosonde
    Local time
    Diurnal temperature variation
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    Low latitude
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    Radio occultation
    Magnetic dip
    Peculiarities of daytime and nighttime Pi 2 pulsations at the dip equator are examined by using multipoint measurements from the 210° magnetic meridian (MM) magnetometer network. We found that during daytime the amplitude of Pi 2 pulsations at the dip equator is enhanced, and the phase lags ∼ 34° behind those at low‐latitude (magnetic latitude Φ = 19.5‐46.2°) stations. On the other hand, during nighttime the amplitude of Pi 2 pulsations at the dip equator is depressed, and the phase lags ∼ 18° behind those at the lower latitudes. Because the zonal ionospheric conductivity at the dip equator is much higher than that at the off‐dip equator region, Pi 2 signals are expected to be distorted more effectively at the dip equator. The observations imply that the daytime and nighttime Pi 2 pulsations in the equatorial and low‐latitude regions can be explained by invoking an instantaneous penetration of electric field variations from the nightside polar ionosphere to the dayside equatorial ionosphere, and a direct incidence of compressional oscillations from the nightside inner magnetosphere, respectively.
    Magnetic dip
    Plasmasphere
    Citations (46)
    Two induction magnetometers have been installed at Zhongshan Station and Davis Station, Antarctica respectively. We adopt with cross-spectral analysis technique to analyze the data of the two induction magnetometers, in June, September, December 1996 and March 1997. to investigate the Pc3 frequency range pulsation occurrence and propagation characteristics in the cusp latitudes. The results are summarized as following: At Zhongshan-Davis Stations, the Pc3 frequency range pulsations occur mainly around the local noon/ local magnetic noon and local magnetic midnight respectively. In daytime, the pulsations have a seasonal variation in amplitude, occurrence and temporal range, all of them are sma1lest in winter. But in nighttime, the pulsations have no such a variation. The pu1sation amplitude in nighttime is much larger than the one in daytime all oveI the year. The pulsation propagating direction is mainly western in daytime and irregularly in nighttime. It can be thought that the different sources of the pulsation and the ionospheric electric conductivity are mainly responsible for these characteristics.
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    Ionosonde
    Critical frequency
    Geomagnetic latitude
    Local time
    Low latitude
    Universal Time