Abstract:Previous investigations of ionospheric storm‐enhanced density (SED) and tongue of ionization (TOI) focused mostly on the behavior of TOI during intense geomagnetic storms. Little attention has been paid to the spatial and temporal variations of TOI during weak to moderate geomagnetic disturbed conditions. In this paper we investigate the source and development of TOI during a moderate geomagnetic storm on 14 October 2012. Multi‐instrumental observations including GPS total electron content (TEC), Defense Meteo… Show more
“…Near the geomagnetic poles, the vertical plasma transport due to the horizontal thermospheric wind is zeroed. Our results are in agreement with previous findings by Liu et al (), Liu, Wang, Burns, Solomon, et al (). These authors have demonstrated that the TOI is enhanced due to equatorward upwelling of plasma at the dayside subauroral latitudes in the region of plasma accumulation before its removal to the polar cap.…”
Section: Resultssupporting
confidence: 94%
“…Sojka et al () reported that under conditions of enhanced magnetospheric convection, TOI is more pronounced. The main characteristics of the TOI occurrence during strong geomagnetic storms have been studied using multi‐instrumental observations and theoretical models (e.g., Foster et al, ; David et al, ; Liu et al, , Liu, Wang, Burns, Solomon, et al, ; Liu, Wang, Burns, Yue, et al, ; Thomas et al, ). Often, occurrence of TOI is linked to another storm time plasma feature—SED, a localized plume‐like increase of ionospheric electron density (particularly the total electron content [TEC]), which is transported poleward from a source region at middle latitudes (Coster & Scone, ; Foster, ).…”
We present the observational and modeling study focused on the major factors determining the spatiotemporal structure of the high‐latitude ionospheric plasma density enhancement—the tongue of ionization (TOI) structure—during the 2015 St. Patrick's Day geomagnetic storm. We use the Global Self‐consistent Model of the Thermosphere, Ionosphere, Protonosphere (GSM TIP) to reproduce the plasma density distribution, and the results are compared with the observational data as deduced from the ground‐based global positioning system total electron content and in situ plasma probe measurements at different altitudes. Both the simulation and observation results show that a large‐scale TOI‐like structure of enhanced plasma density extends from the dayside midlatitude region toward the central polar cap along the antisunward cross‐polar convection flow. We reveal an important role of the clockwise convection cell rotation for the modification of TOI structure. According to model results during the storm main phase, the neutral thermospheric composition, particularly the “tongue” in n(N2), modifies the spatial structure of TOI in such a way that (1) the near‐pole region of enhanced plasma density is shifted to the duskside and, (2) at F region heights, the TOI is split into the dusk and dawn branches. The signature of TOI in the topside ionosphere considerably differs from that in the F region because of a lesser influence of the neutral composition changes at higher altitudes. Model results revealed that at plasmaspheric heights, the TOI structure appears in both the dawn and dusk convection cells.
“…Near the geomagnetic poles, the vertical plasma transport due to the horizontal thermospheric wind is zeroed. Our results are in agreement with previous findings by Liu et al (), Liu, Wang, Burns, Solomon, et al (). These authors have demonstrated that the TOI is enhanced due to equatorward upwelling of plasma at the dayside subauroral latitudes in the region of plasma accumulation before its removal to the polar cap.…”
Section: Resultssupporting
confidence: 94%
“…Sojka et al () reported that under conditions of enhanced magnetospheric convection, TOI is more pronounced. The main characteristics of the TOI occurrence during strong geomagnetic storms have been studied using multi‐instrumental observations and theoretical models (e.g., Foster et al, ; David et al, ; Liu et al, , Liu, Wang, Burns, Solomon, et al, ; Liu, Wang, Burns, Yue, et al, ; Thomas et al, ). Often, occurrence of TOI is linked to another storm time plasma feature—SED, a localized plume‐like increase of ionospheric electron density (particularly the total electron content [TEC]), which is transported poleward from a source region at middle latitudes (Coster & Scone, ; Foster, ).…”
We present the observational and modeling study focused on the major factors determining the spatiotemporal structure of the high‐latitude ionospheric plasma density enhancement—the tongue of ionization (TOI) structure—during the 2015 St. Patrick's Day geomagnetic storm. We use the Global Self‐consistent Model of the Thermosphere, Ionosphere, Protonosphere (GSM TIP) to reproduce the plasma density distribution, and the results are compared with the observational data as deduced from the ground‐based global positioning system total electron content and in situ plasma probe measurements at different altitudes. Both the simulation and observation results show that a large‐scale TOI‐like structure of enhanced plasma density extends from the dayside midlatitude region toward the central polar cap along the antisunward cross‐polar convection flow. We reveal an important role of the clockwise convection cell rotation for the modification of TOI structure. According to model results during the storm main phase, the neutral thermospheric composition, particularly the “tongue” in n(N2), modifies the spatial structure of TOI in such a way that (1) the near‐pole region of enhanced plasma density is shifted to the duskside and, (2) at F region heights, the TOI is split into the dusk and dawn branches. The signature of TOI in the topside ionosphere considerably differs from that in the F region because of a lesser influence of the neutral composition changes at higher altitudes. Model results revealed that at plasmaspheric heights, the TOI structure appears in both the dawn and dusk convection cells.
“…Resultant antisunward convection in the middle of the polar cap can lead to (segmented or unsegmented) TOI [e.g., Zhang et al , ; Walsh et al , ], which is elongated across different L shells by definition. Note that TOIs can occur during strong as well as moderate to weak geomagnetic storms [e.g., Liu et al , , and references therein]. As our study imposes no constraints on geomagnetic activity, TOIs will also contribute to the statistics in the polar cap, as shown in Figures and .…”
In this study, we investigate the climatology of high‐latitude total electron content (TEC) variations as observed by the dual‐frequency Global Navigation Satellite Systems (GNSS) receivers onboard the Swarm satellite constellation. The distribution of TEC perturbations as a function of geographic/magnetic coordinates and seasons reasonably agrees with that of the Challenging Minisatellite Payload observations published earlier. Categorizing the high‐latitude TEC perturbations according to line‐of‐sight directions between Swarm and GNSS satellites, we can deduce their morphology with respect to the geomagnetic field lines. In the Northern Hemisphere, the perturbation shapes are mostly aligned with the L shell surface, and this anisotropy is strongest in the nightside auroral (substorm) and subauroral regions and weakest in the central polar cap. The results are consistent with the well‐known two‐cell plasma convection pattern of the high‐latitude ionosphere, which is approximately aligned with L shells at auroral regions and crossing different L shells for a significant part of the polar cap. In the Southern Hemisphere, the perturbation structures exhibit noticeable misalignment to the local L shells. Here the direction toward the Sun has an additional influence on the plasma structure, which we attribute to photoionization effects. The larger offset between geographic and geomagnetic poles in the south than in the north is responsible for the hemispheric difference.
“…Storm time, single‐site observations from the Millstone Hill Incoherent Radar (ISR) frequently show dramatic F region electron density enhancements around the duskside, which is termed the “dusk effect” [e.g., Papagiannis et al ., ; Mendillo et al ., ; Evans , ; Anderson , ; Buonsanto , , , ]. Based on Millstone Hill ISR 2‐D electron density measurements, Foster [] renamed this phenomenon SED, which is typically characterized by a latitudinally distinct region of sunward convection F region plasma, high electron densities, an elevated F region peak, a significantly enhanced topside ionosphere, and low electron temperatures near sunset at middle latitudes [ Foster , ; Liu et al ., , ]. Cherniak and Zakharenkova [] reported that high‐latitude ionospheric irregularities tend to occur in the edge of SED/TOI having steep ionospheric density gradients during the St. Patrick's Day event in 2015.…”
Section: Introductionmentioning
confidence: 99%
“…In some literatures, people do not distinguish between SED and TOI since these two are quite similar but occur at different latitudes. However, Liu et al [2015] reported that TOI can also occur during geomagnetic quiet or weakly disturbed conditions at favorable universal local times independent of SED occurrence. TOI tends to form during the universal times when high-latitude two-cell convection patterns are closer to solar-produced middle-latitude plasma source region, facilitating the poleward plasma transportations.…”
There are still uncertainties regarding the formation mechanisms for storm‐enhanced density (SED) in the high and subauroral latitude ionosphere. In this work, we deploy the Thermosphere Ionosphere Electrodynamic General Circulation Model (TIEGCM) and GPS total electron content (TEC) observations to identify the principle mechanisms for SED and the tongue of ionization (TOI) through term‐by‐term analysis of the ion continuity equation and also identify the advantages and deficiencies of the TIEGCM in capturing high‐latitude and subauroral latitude ionospheric fine structures for the two geomagnetic storm events occurring on 17 March 2013 and 2015. Our results show that in the topside ionosphere, upward E × B ion drifts are most important in SED formation and are offset by antisunward neutral winds and downward ambipolar diffusion effects. In the bottomside F region ionosphere, neutral winds play a major role in generating SEDs. SED signature in TEC is mainly caused by upward E × B ion drifts that lift the ionosphere to higher altitudes where chemical recombination is slower. Horizontal E × B ion drifts play an essential role in transporting plasma from the dayside convection throat region to the polar cap to form TOIs. Inconsistencies between model results and GPS TEC data were found: (1) GPS relative TEC difference between storm time and quiet time has “holes” in the dayside ion convection entrance region, which do not appear in the model results. (2) The model tends to overestimate electron density enhancements in the polar region. Possible causes for these inconsistencies are discussed in this article.
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