2013
DOI: 10.1007/s11141-013-9437-x
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Structure of the Electric Field of a High-Power Radio Wave in the Outer Ionosphere

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Cited by 11 publications
(16 citation statements)
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References 30 publications
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“…The results from the reconstruction of the ionospheric electron density distribution indicate that as f 0 approaches foF2, density troughs may form that stretch along the entire F2 layer. Ray tracing calculations suggest that in these troughs the plasma became locally underdense for O-mode propagation so that pump energy could be transmitted through the F-region density peak into the topside ionosphere with the pump wave propagating along the geomagnetic field, thus arriving at similar conclusions as those of Frolov et al (2013). James et al (2017) reported transmissions from the Sura facility to CASSIOPE at an altitude of about 1300 km, for foF2 ∼ 0.1 MHz above f 0 of the transmitted O-mode wave.…”
Section: Discussionmentioning
confidence: 78%
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“…The results from the reconstruction of the ionospheric electron density distribution indicate that as f 0 approaches foF2, density troughs may form that stretch along the entire F2 layer. Ray tracing calculations suggest that in these troughs the plasma became locally underdense for O-mode propagation so that pump energy could be transmitted through the F-region density peak into the topside ionosphere with the pump wave propagating along the geomagnetic field, thus arriving at similar conclusions as those of Frolov et al (2013). James et al (2017) reported transmissions from the Sura facility to CASSIOPE at an altitude of about 1300 km, for foF2 ∼ 0.1 MHz above f 0 of the transmitted O-mode wave.…”
Section: Discussionmentioning
confidence: 78%
“…Since in our case transionospheric propagation with f 0 < foF2 was observed, the absorption cannot have been too strong. We therefore suggest that L-and associated Z-mode propagation cannot be ruled out for the cases discussed by Frolov et al (2013). L-mode propagation would explain why transionospheric propagation was indeed observed near magnetic zenith and only for foF2 − f 0 f e /2, as the L-mode has its cutoff at f p ≈ f 0 + f e /2 and is evanescent for higher f p .…”
Section: Discussionmentioning
confidence: 84%
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“…It may have a strong effect on propagation of radio waves of different frequency ranges and, as was demonstrated in [32], on transmission of the pump wave into the topside ionosphere. …”
Section: Characteristics Of the Cavity With Depleted Plasma Density (mentioning
confidence: 89%