Morphology of sporadic E layer retrieved from COSMIC GPS radio occultation measurements: Wind shear theory examination

On the basis of the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC)‐measured fluctuations in the signal‐to‐noise ratio and excess phase of the GPS signal piercing through ionospheric sporadic E (Es) layers, the general morphologies of these layers are presented for t...

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Veröffentlicht in:Journal of geophysical research. Space physics 2014-03, Vol.119 (3), p.2117-2136
Hauptverfasser: Chu, Y. H., Wang, C. Y., Wu, K. H., Chen, K. T., Tzeng, K. J., Su, C. L., Feng, W., Plane, J. M. C.
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container_issue 3
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container_title Journal of geophysical research. Space physics
container_volume 119
creator Chu, Y. H.
Wang, C. Y.
Wu, K. H.
Chen, K. T.
Tzeng, K. J.
Su, C. L.
Feng, W.
Plane, J. M. C.
description On the basis of the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC)‐measured fluctuations in the signal‐to‐noise ratio and excess phase of the GPS signal piercing through ionospheric sporadic E (Es) layers, the general morphologies of these layers are presented for the period from July 2006 to May 2011. It is found that the latitudinal variation in the Es layer occurrence is substantially geomagnetically controlled, most frequent in the summer hemisphere within the geomagnetic latitude region between 10° and 70° and very rare in the geomagnetic equatorial zone. Model simulations show that the summer maximum (winter minimum) in the Es layer occurrence is very likely attributed to the convergence of the Fe+ concentration flux driven by the neutral wind. In addition to seasonal and spatial distributions, the height‐time variations in the Es layer occurrence in the midlatitude (>30°) region in summer and spring are primarily dominated by the semidiurnal tides, which start to appear at local time around 6 and 18 h in the height range 110–120 km and gradually descend at a rate of about 0.9–1.6 km/h. In the low‐latitude (
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H. ; Wang, C. Y. ; Wu, K. H. ; Chen, K. T. ; Tzeng, K. J. ; Su, C. L. ; Feng, W. ; Plane, J. M. C.</creator><creatorcontrib>Chu, Y. H. ; Wang, C. Y. ; Wu, K. H. ; Chen, K. T. ; Tzeng, K. J. ; Su, C. L. ; Feng, W. ; Plane, J. M. C.</creatorcontrib><description>On the basis of the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC)‐measured fluctuations in the signal‐to‐noise ratio and excess phase of the GPS signal piercing through ionospheric sporadic E (Es) layers, the general morphologies of these layers are presented for the period from July 2006 to May 2011. It is found that the latitudinal variation in the Es layer occurrence is substantially geomagnetically controlled, most frequent in the summer hemisphere within the geomagnetic latitude region between 10° and 70° and very rare in the geomagnetic equatorial zone. Model simulations show that the summer maximum (winter minimum) in the Es layer occurrence is very likely attributed to the convergence of the Fe+ concentration flux driven by the neutral wind. In addition to seasonal and spatial distributions, the height‐time variations in the Es layer occurrence in the midlatitude (&gt;30°) region in summer and spring are primarily dominated by the semidiurnal tides, which start to appear at local time around 6 and 18 h in the height range 110–120 km and gradually descend at a rate of about 0.9–1.6 km/h. In the low‐latitude (&lt;30°) region, the diurnal tide dominates. The Horizontal Wind Model (HWM07) indicates that the height‐time distribution of Es layers at middle latitude (30°–60°) is highly coincident with the zonal neutral wind shear. However, Es layer occurrences in low‐latitude and equatorial regions do not correlate well with the zonal wind shear. 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It is found that the latitudinal variation in the Es layer occurrence is substantially geomagnetically controlled, most frequent in the summer hemisphere within the geomagnetic latitude region between 10° and 70° and very rare in the geomagnetic equatorial zone. Model simulations show that the summer maximum (winter minimum) in the Es layer occurrence is very likely attributed to the convergence of the Fe+ concentration flux driven by the neutral wind. In addition to seasonal and spatial distributions, the height‐time variations in the Es layer occurrence in the midlatitude (&gt;30°) region in summer and spring are primarily dominated by the semidiurnal tides, which start to appear at local time around 6 and 18 h in the height range 110–120 km and gradually descend at a rate of about 0.9–1.6 km/h. In the low‐latitude (&lt;30°) region, the diurnal tide dominates. The Horizontal Wind Model (HWM07) indicates that the height‐time distribution of Es layers at middle latitude (30°–60°) is highly coincident with the zonal neutral wind shear. However, Es layer occurrences in low‐latitude and equatorial regions do not correlate well with the zonal wind shear. Key Points Examination of Es layer summer maximum phenomenon Global distribution of COSMIC‐retrieved Es layer Es layer formation and wind shear mechanism</description><subject>Diurnal variations</subject><subject>Geomorphology</subject><subject>Geophysics</subject><subject>GPS radio occultation</subject><subject>Ionosphere</subject><subject>Latitude</subject><subject>Spatial distribution</subject><subject>sporadic E layer</subject><subject>Summer</subject><subject>Wind shear</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp90c9P2zAUB_BoYtIQcOMPsMRlBwL-EbvObqUqAdSO0W4rN8txXlZDEhc7YeS_X1hhQhzmiy3r8316Ty-KDgk-IRjTU4oJuxpjkiZs9CHapUSkcZpguvP6ZhJ_ig5CuMPDkcMX4bvR49z5zdpV7lePXInCxnldWIOmqNI9eOSh9RYeoUCldzWaXC_nlxOUfVuiZ-eQM6arWt1a16AadOg81NC04Qta2aZAYQ3ao3YNzvcInnRtm792P_pY6irAwcu9F_04n36fXMSz6-xyMp7FhlMuYqZxTo0pCOUAshwViWC8LIikRBcJoTrPJUkhpzI3kok8F7IskhQLEIYawthe9Hlbd-PdQwehVbUNBqpKN-C6oAinSUIpTdKBHr2jd67zzdCdIoJJhglP8aCOt8p4F4KHUm28rbXvFcHqeQ_q7R4Gzrb8t62g_69VV9lizPEwxpCKtykbWnj6l9L-XokRG3G1-pqpFRU_F9nNrTpjfwBzV5hr</recordid><startdate>201403</startdate><enddate>201403</enddate><creator>Chu, Y. 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Space physics</jtitle><addtitle>J. Geophys. Res. Space Physics</addtitle><date>2014-03</date><risdate>2014</risdate><volume>119</volume><issue>3</issue><spage>2117</spage><epage>2136</epage><pages>2117-2136</pages><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>On the basis of the Constellation Observing System for Meteorology, Ionosphere, and Climate (COSMIC)‐measured fluctuations in the signal‐to‐noise ratio and excess phase of the GPS signal piercing through ionospheric sporadic E (Es) layers, the general morphologies of these layers are presented for the period from July 2006 to May 2011. It is found that the latitudinal variation in the Es layer occurrence is substantially geomagnetically controlled, most frequent in the summer hemisphere within the geomagnetic latitude region between 10° and 70° and very rare in the geomagnetic equatorial zone. Model simulations show that the summer maximum (winter minimum) in the Es layer occurrence is very likely attributed to the convergence of the Fe+ concentration flux driven by the neutral wind. In addition to seasonal and spatial distributions, the height‐time variations in the Es layer occurrence in the midlatitude (&gt;30°) region in summer and spring are primarily dominated by the semidiurnal tides, which start to appear at local time around 6 and 18 h in the height range 110–120 km and gradually descend at a rate of about 0.9–1.6 km/h. In the low‐latitude (&lt;30°) region, the diurnal tide dominates. The Horizontal Wind Model (HWM07) indicates that the height‐time distribution of Es layers at middle latitude (30°–60°) is highly coincident with the zonal neutral wind shear. However, Es layer occurrences in low‐latitude and equatorial regions do not correlate well with the zonal wind shear. 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subjects Diurnal variations
Geomorphology
Geophysics
GPS radio occultation
Ionosphere
Latitude
Spatial distribution
sporadic E layer
Summer
Wind shear
title Morphology of sporadic E layer retrieved from COSMIC GPS radio occultation measurements: Wind shear theory examination
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