Abstract:Abstract. The VHF radars have been extensively used to investigate the structures and dynamics of equatorial Spread F (ESF) irregularities. However, unambiguous identification of the nature of the structures in terms of plasma depletion or enhancement requires another technique, as the return echo measured by VHF radar is proportional to the square of the electron density fluctuations. In order to address this issue, co-ordinated radar backscatter and thermospheric airglow intensity measurements were carried o… Show more
“…The nighttime airglow emissions (OI 630.0 nm and 777.4 nm) from thermosphere altitudes (∼250 km and F region peak altitude) have been monitored using a temperature controlled narrow band (0.3 nm) optical photometer whose field of view (3 • ) was chosen to nearly coincide with radar beam width. The details of this photometer (Sekar et al, 2004) and coordinated observations (Chakrabarty et al, 2005(Chakrabarty et al, , 2006 are available in the literature. In addition to these techniques, the layer height movements of the F-region over the dip equator which correspond to zonal electric fields were obtained from the ionosonde observations located at Thumba.…”
Abstract. Plasma irregularity structures associated with an Equatorial Spread-F (ESF) event were recorded by the Indian VHF Radar on 26-27 April 2006 near midnight hours. The plasma structures were found to be isolated without having bottomside structure. They moved predominantly downward and the structures were found to be less turbulent than their post-sunset counterparts. However, the structures were characterized by meter-scale size irregularities. These structures are identified for the first time as plasma depletion structures using simultaneous, collocated measurements of OI 630.0 nm airglow intensity variations. The variation of the base height of ionospheric F layer over dip equator is also presented to buttress the result. Further, these plasma structures are shown to be "active fossil bubbles".
“…The nighttime airglow emissions (OI 630.0 nm and 777.4 nm) from thermosphere altitudes (∼250 km and F region peak altitude) have been monitored using a temperature controlled narrow band (0.3 nm) optical photometer whose field of view (3 • ) was chosen to nearly coincide with radar beam width. The details of this photometer (Sekar et al, 2004) and coordinated observations (Chakrabarty et al, 2005(Chakrabarty et al, , 2006 are available in the literature. In addition to these techniques, the layer height movements of the F-region over the dip equator which correspond to zonal electric fields were obtained from the ionosonde observations located at Thumba.…”
Abstract. Plasma irregularity structures associated with an Equatorial Spread-F (ESF) event were recorded by the Indian VHF Radar on 26-27 April 2006 near midnight hours. The plasma structures were found to be isolated without having bottomside structure. They moved predominantly downward and the structures were found to be less turbulent than their post-sunset counterparts. However, the structures were characterized by meter-scale size irregularities. These structures are identified for the first time as plasma depletion structures using simultaneous, collocated measurements of OI 630.0 nm airglow intensity variations. The variation of the base height of ionospheric F layer over dip equator is also presented to buttress the result. Further, these plasma structures are shown to be "active fossil bubbles".
“…The detailed description of this structure in comparison with the observation on non ESF night along with the corresponding airglow signatures in the vertical direction have been discussed in a previous communication (Sekar et al, 2004). Some of the plume structures were shown to be plasma enhancements (Sekar et al, 2004). However, the airglow observations in the eastward (45 • elevation) direction were not considered earlier and are included in Fig.…”
Section: Observationsmentioning
confidence: 96%
“…It is noted that, unlike the previous two cases, this day was magnetically quiet (A P =3, F 10.7 =97). The detailed description of this structure in comparison with the observation on non ESF night along with the corresponding airglow signatures in the vertical direction have been discussed in a previous communication (Sekar et al, 2004). Some of the plume structures were shown to be plasma enhancements (Sekar et al, 2004).…”
Section: Observationsmentioning
confidence: 99%
“…The details of the multi-wavelength scanning photometer for airglow studies during nighttime have been discussed in a previous communication (Sekar et al, 2004). Temperaturetuned, narrow band (band width ∼0.3 nm) interference filters are used in this photometer.…”
Section: Methodsmentioning
confidence: 99%
“…Thus the comparative studies with various techniques are useful in obtaining physical insight of ESF. In the recent past, comparison between the narrow-band optical measurements of thermospheric airglow emissions and the VHF radar measurements revealed the presence of plasma enhancement (Sekar et al, 2004) extending beyond 350 km and an evidence for fossil bubbles turning active (Sekar et al, 2007) was obtained. In addition, simultaneous triggering of ESF at two zonally separated locations during storm time was identified (Chakrabarty et al, 2006;Sekar and Chakrabarty , 2008) using bi-directional airglow and VHF radar observations.…”
Abstract. Co-ordinated campaigns have been conducted from Gadanki (13.5 • N, 79.2 • E, dip lat 6.4 • N) by operating simultaneously the Indian MST radar in ionospheric coherent backscatter mode and by monitoring thermosphere airglow line emissions (630.0 nm and 777.4 nm) using a narrow band multi-wavelength scanning photometer during JanuaryMarch for the past five years (2003)(2004)(2005)(2006)(2007) and also during April 2006, as a special campaign. Simultaneous radar and optical observations reveal optical signatures corresponding to a variety of equatorial spread F (ESF) structures. The optical signatures corresponding to ESF structures with wavelike bottomside modulations with plasma plumes, confined bottomside flat and wavelike structures, vertically extended plume structure in the absence of bottomside structure apart from the classical plasma depletions and enhancements are obtained during these campaigns. The plasma depletions and enhancements were identified using optical measurements. In addition, estimations of zonal wavelength of the bottomside structures and the inference of shears in the zonal plasma drift in the presence of confined structures, were carried out using bi-directional airglow measurements. Furthermore, it is found that the vertical columnar intensity of OI 630.0 nm airglow exceeded the slanted columnar intensity in the presence of large bottomside structure. The need for the appropriate physical mechanisms for some of the ESF structures and their characterizations with optical observations are discussed.
VHF radar echoes from the valley region plasma irregularities, displaying ascending pattern, are often observed during the active phase of equatorial plasma bubble in the close vicinity of the geomagnetic equator and have been attributed to bubble-related fringe field effect. These irregularities however are not observed at a few degrees away from the equator. In this paper, we attempt to understand this contrasting observational result by comparing fringe field at the geomagnetic equator and low latitudes. We use parallel plate capacitor analogy of equatorial plasma bubble and choose a few capacitor configurations, consistent with commonly observed dimension and magnetic field-aligned property of plasma bubble, for computing fringe field. Results show that fringe field decreases significantly with decreasing altitude as expected. Further, fringe field decreases remarkably with latitude, which clearly indicates the role of magnetic field-aligned property of plasma bubble in reducing the magnitude of fringe field at low latitudes compared to that at the geomagnetic equator. The results are presented and discussed in the light of current understanding of plasma bubble-associated fringe field-induced plasma irregularities in the valley region.
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