1978
DOI: 10.1029/ar029p0200
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Antarctic ionospheric research

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Cited by 59 publications
(44 citation statements)
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References 67 publications
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“…The ionosonde results in the southern hemisphere in Figures 3a, 5a, and 5d reveal that the nighttime electron density enhancements prefer to appear during summer months than winter months, which are consistent with the previous studies [ Bellchambers and Piggott , 1958; Penndorf , 1965; Dudeney and Piggott , 1978; Burns et al , 2008; Lin et al , 2009; Liu et al , 2010]. Liu et al [2010] and Chen et al [2011] reported that the neutral wind is an important driver for the MSNA formation.…”
Section: Discussionsupporting
confidence: 90%
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“…The ionosonde results in the southern hemisphere in Figures 3a, 5a, and 5d reveal that the nighttime electron density enhancements prefer to appear during summer months than winter months, which are consistent with the previous studies [ Bellchambers and Piggott , 1958; Penndorf , 1965; Dudeney and Piggott , 1978; Burns et al , 2008; Lin et al , 2009; Liu et al , 2010]. Liu et al [2010] and Chen et al [2011] reported that the neutral wind is an important driver for the MSNA formation.…”
Section: Discussionsupporting
confidence: 90%
“… Burns et al , 2008, and references therein], recent renewed observations give wider extended coverage of the anomaly and prompt us to investigate the physical mechanism based on these new observations. According to the previous studies, the possible physical mechanisms of MSNA are photoionization of solar ultraviolet radiation [ Sojka et al , 1985; Horvath and Essex , 2003], equatorward neutral winds [ Park , 1971; Dudeney and Piggott , 1978; Su et al , 1994; Horvath and Essex , 2003; He et al , 2009; Thampi et al , 2009; Liu et al , 2010; Lin et al , 2010; Chen et al , 2011], the magnetic field configuration and offset effect [ Kohl and King , 1967; Dudeney and Piggott , 1978; Horvath , 2006; Lin et al , 2009, 2010; Liu et al , 2010; Chen et al , 2011], and the downward diffusion of the plasmaspheric plasma [ Park , 1971; Bailey et al , 1991; Burns et al , 2008; Liu et al , 2010; Chen et al , 2011]. Recently, Chen et al [2011] used a theoretical model, SAMI2 model [ Huba et al , 2000], to reproduce the integrated three‐dimensional WSA electron density structure and examine the causal mechanisms of WSA formation.…”
Section: Discussionmentioning
confidence: 99%
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“…Thus the strength of plasma drift becomes strongest at 45° dip angle (I) [ Khol and King , 1967; Dudeney and Piggott , 1978], and remains large at dip angles between 20°–70° corresponding to dip latitudes of 10°–54° [ Titheridge , 1995]. During the night, upward ionospheric drifts are produced by the equatorward neutral winds that move the ionization to higher altitudes along the magnetic field lines where the loss rates are lower and thus increase the electron density and TEC.…”
Section: Tec Space Weather Observations and Discussionmentioning
confidence: 99%
“… Horvath and Essex [2003] detected just about the complete image of both phenomena during the 1998/1999 high‐sunspot summer period by utilizing the TOPEX/Poseidon technique. They pointed out first that the real size of the Weddell Sea Anomaly is much larger than was thought previously by other researchers based upon their land‐based ionosonde observations at Faraday, the name of the ionosonde station at Argentine Islands (295.7°E; −65.3°N, geographic) that is now called Vernadsky, in Antarctica providing only a limited data coverage [ Bellchambers and Piggott , 1958; Penndorft , 1965; Dudeney and Piggott , 1978; Clilverd et al , 1991]. With a series of TOPEX TEC maps, Horvath and Essex [2003] demonstrated that larger part of the Weddell Sea Anomaly is situated west of Argentine Islands over the Bellingshausen Sea, not over the Weddell Sea that is east of Argentine Islands, and concluded that it should be called the Bellingshausen Sea Anomaly.…”
Section: Introductionmentioning
confidence: 99%