2008
DOI: 10.5194/angeo-26-2427-2008
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On the diurnal variability in F2-region plasma density above the EISCAT Svalbard radar

Abstract: Abstract. Two long runs of EISCAT Svalbard Radar (ESR), in February 2001 and October 2002, have been analysed with respect to variability in the F2 region peak density and altitude. The diurnal variation in the F2 peak density exhibits one maximum around 12:00 MLT and another around 23:00 MLT, consistent with solar wind controlled transport of EUV ionized plasma across the polar cap from day to night. High density plasma patch material is drawn in through the cusp inflow region independent of IMF B Y . There i… Show more

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Cited by 67 publications
(102 citation statements)
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References 21 publications
(27 reference statements)
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“…The enhancement around noon is visible mainly in the NYA map as an expected cusp effect due to the field of view of the station. To this enhancement contributes also the polar cap patches that form in the cusp and enters the polar cap in cusp inflow region (Moen et al, 2008). During midnight the enhancement and the asymmetry are evident also in the auroral stations (HAM and BRO), while NOT data contribute weakly to the midnight enhancement, maybe due to the equatorward boundary of the very disturbed oval.…”
Section: Phase Scintillationmentioning
confidence: 95%
“…The enhancement around noon is visible mainly in the NYA map as an expected cusp effect due to the field of view of the station. To this enhancement contributes also the polar cap patches that form in the cusp and enters the polar cap in cusp inflow region (Moen et al, 2008). During midnight the enhancement and the asymmetry are evident also in the auroral stations (HAM and BRO), while NOT data contribute weakly to the midnight enhancement, maybe due to the equatorward boundary of the very disturbed oval.…”
Section: Phase Scintillationmentioning
confidence: 95%
“…Patches become particularly large during geomagnetic storms (called tongue of ionization) and form a channel of enhanced density from the dayside and nightside auroral oval across the polar cap (Foster et al 2005). The IMF By also controls dawn-dusk motion of patches (Moen et al 2008a;Hosokawa et al 2009). Convection within the polar cap is often assumed to consist of relatively uniform anti-sunward flow with a typical speed of several hundreds of m/s (e.g., MacDougall and Jayachandran 2001).…”
Section: Introductionmentioning
confidence: 99%
“…There is a possibility that patches formed in the cusp and convected towards the night-time auroral oval also contribute to scintillation and cycle slips. The asymmetry of the polar cap patches distribution around magnetic midnight has been recently discussed by Moen et al (2008). Regions of most frequent occurrence of scintillation as a function of magnetic latitude and magnetic local time (MLT) are subject of ongoing investigation to be presented in the future publication.…”
Section: Gps Scintillation In the Auroral And Cusp Regionsmentioning
confidence: 99%