2020
DOI: 10.1016/j.jastp.2020.105200
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Global ionosonde and GPS radio occultation sporadic-E intensity and height comparison

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Cited by 18 publications
(41 citation statements)
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“…where the TEC perturbation is divided by an effective path length of 176 km corresponding to an effective path through a cylinder with a vertical thickness of ∆R = 0.6 km located at a radial distance R from the center of Earth [26]. The effective path length is derived from an assumed geometry of a cylinder centered around the tangent point [31].…”
Section: Gooch Methodsmentioning
confidence: 99%
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“…where the TEC perturbation is divided by an effective path length of 176 km corresponding to an effective path through a cylinder with a vertical thickness of ∆R = 0.6 km located at a radial distance R from the center of Earth [26]. The effective path length is derived from an assumed geometry of a cylinder centered around the tangent point [31].…”
Section: Gooch Methodsmentioning
confidence: 99%
“…Instead of directly comparing ionograms and GPS-RO crossings within a short time window (e.g., 30 min between ionogram and crossing as outlined in Ref. [26]), here we compare rates averaged over TOD for the areas surrounding each ionosonde site. A direct comparison of each GPS-RO crossing within 170 km of a site certainly has merit as it ensures the measurements are taken at nearly the same time and location.…”
Section: Comparison Criteriamentioning
confidence: 99%
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“…GPS radio occultation (RO) measurements provide a dense set of global measurements and have recently been used to estimate global E s occurrence rates [29,30,33,34]. However, the direct relationship between GPS-RO measurements to sporadic-E parameters and intensity are difficult to determine because of the unknown length, orientation, and vertical thickness of the sporadic-E layers [35].…”
Section: Introductionmentioning
confidence: 99%