Postmidnight ionospheric troughs in summer at high latitudes
In this article we identify possible mechanisms for the formation of postmidnight ionospheric troughs during summer, in sunlit plasma. Four events were identified in measurements of European Incoherent Scatter and ESR radars during CP3 experiments, when the ionosphere was scanned in a meridional pla...
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Veröffentlicht in: | Journal of geophysical research. Space physics 2016-12, Vol.121 (12), p.12,171-12,185 |
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creator | Voiculescu, M. Nygrén, T. Aikio, A. T. Vanhamäki, H. Pierrard, V. |
description | In this article we identify possible mechanisms for the formation of postmidnight ionospheric troughs during summer, in sunlit plasma. Four events were identified in measurements of European Incoherent Scatter and ESR radars during CP3 experiments, when the ionosphere was scanned in a meridional plan. The spatial and temporal variation of plasma density, ion, and electron temperatures were analyzed for each of the four events. Super Dual Auroral Radar Network plasma velocity measurements were added, when these were available. For all high‐latitude troughs the ion temperatures are high at density minima (within the trough), at places where the convection plasma velocity is eastward and high. There is no significant change in electron temperature inside the trough, regardless of its temporal evolution. We find that troughs in sunlit plasma form in two steps: the trough starts to form when energetic electron precipitation leads to faster recombination in the F region, and it deepens when entering a region with high eastward flow, producing frictional heating and further depleting the plasma. The high‐latitude plasma convection plays an important role in formation and evolution of troughs in the postmidnight sector in sunlit plasma. During one event a second trough is identified at midlatitudes, with different characteristics, which is most likely produced by a rapid subauroral ion drift in the premidnight sector.
Key Points
The high‐latitude plasma convection plays a role in formation and evolution of troughs in the postmidnight sector in sunlit plasma
Ion temperatures are high at density minima (within the trough) at places where the convection plasma velocity is eastward and high
A two‐step process leads to formation of troughs in sunlit plasma: (1) energetic electron precipitation and (2) frictional heating |
doi_str_mv | 10.1002/2016JA023360 |
format | Article |
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Key Points
The high‐latitude plasma convection plays a role in formation and evolution of troughs in the postmidnight sector in sunlit plasma
Ion temperatures are high at density minima (within the trough) at places where the convection plasma velocity is eastward and high
A two‐step process leads to formation of troughs in sunlit plasma: (1) energetic electron precipitation and (2) frictional heating</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1002/2016JA023360</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Convection ; Convection heating ; Electron energy ; Electron precipitation ; Electron temperature ; Electron temperatures ; Evolution ; F region ; F region trough ; Formations ; Geophysics ; Heating ; ion heating ; Ion temperature ; Ionosphere ; ionospheric convection ; Latitude ; Minima ; Plasma ; Plasma convection ; Plasma density ; Plasmas (physics) ; Radar ; Radar networks ; Scattering ; Troughs</subject><ispartof>Journal of geophysical research. Space physics, 2016-12, Vol.121 (12), p.12,171-12,185</ispartof><rights>2016. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4670-6211b73c1a4156c4b72c2379434c5ef180f15712fe3d91fc6bcac066117276bd3</citedby><cites>FETCH-LOGICAL-c4670-6211b73c1a4156c4b72c2379434c5ef180f15712fe3d91fc6bcac066117276bd3</cites><orcidid>0000-0001-5014-7682 ; 0000-0002-3454-0350 ; 0000-0002-1864-3878 ; 0000-0001-8838-5125</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2F2016JA023360$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2F2016JA023360$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,1433,27924,27925,45574,45575,46409,46833</link.rule.ids></links><search><creatorcontrib>Voiculescu, M.</creatorcontrib><creatorcontrib>Nygrén, T.</creatorcontrib><creatorcontrib>Aikio, A. T.</creatorcontrib><creatorcontrib>Vanhamäki, H.</creatorcontrib><creatorcontrib>Pierrard, V.</creatorcontrib><title>Postmidnight ionospheric troughs in summer at high latitudes</title><title>Journal of geophysical research. Space physics</title><description>In this article we identify possible mechanisms for the formation of postmidnight ionospheric troughs during summer, in sunlit plasma. Four events were identified in measurements of European Incoherent Scatter and ESR radars during CP3 experiments, when the ionosphere was scanned in a meridional plan. The spatial and temporal variation of plasma density, ion, and electron temperatures were analyzed for each of the four events. Super Dual Auroral Radar Network plasma velocity measurements were added, when these were available. For all high‐latitude troughs the ion temperatures are high at density minima (within the trough), at places where the convection plasma velocity is eastward and high. There is no significant change in electron temperature inside the trough, regardless of its temporal evolution. We find that troughs in sunlit plasma form in two steps: the trough starts to form when energetic electron precipitation leads to faster recombination in the F region, and it deepens when entering a region with high eastward flow, producing frictional heating and further depleting the plasma. The high‐latitude plasma convection plays an important role in formation and evolution of troughs in the postmidnight sector in sunlit plasma. During one event a second trough is identified at midlatitudes, with different characteristics, which is most likely produced by a rapid subauroral ion drift in the premidnight sector.
Key Points
The high‐latitude plasma convection plays a role in formation and evolution of troughs in the postmidnight sector in sunlit plasma
Ion temperatures are high at density minima (within the trough) at places where the convection plasma velocity is eastward and high
A two‐step process leads to formation of troughs in sunlit plasma: (1) energetic electron precipitation and (2) frictional heating</description><subject>Convection</subject><subject>Convection heating</subject><subject>Electron energy</subject><subject>Electron precipitation</subject><subject>Electron temperature</subject><subject>Electron temperatures</subject><subject>Evolution</subject><subject>F region</subject><subject>F region trough</subject><subject>Formations</subject><subject>Geophysics</subject><subject>Heating</subject><subject>ion heating</subject><subject>Ion temperature</subject><subject>Ionosphere</subject><subject>ionospheric convection</subject><subject>Latitude</subject><subject>Minima</subject><subject>Plasma</subject><subject>Plasma convection</subject><subject>Plasma density</subject><subject>Plasmas (physics)</subject><subject>Radar</subject><subject>Radar networks</subject><subject>Scattering</subject><subject>Troughs</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqN0UtLw0AQAOBFFCy1N39AwIsHqzO72UfASylaLQVF9Lwkm02zJY-6myD996ZUQTyIc5lh-BhmGELOEa4RgN5QQLGcAWVMwBEZURTJNImBHn_XTMEpmYSwgSHU0EI-IrfPbehqlzduXXaRa5s2bEvrnYk63_brMkSuiUJf19ZHaReVA4uqtHNdn9twRk6KtAp28pXH5O3-7nX-MF09LR7ns9XUxELCVFDETDKDaYxcmDiT1FAmk5jFhtsCFRTIJdLCsjzBwojMpAaEQJRUiixnY3J5mLv17XtvQ6drF4ytqrSxbR80KgXAKBfwDyoUQyYlHejFL7ppe98Mh2hMADlLqGJ_KsWHGxTS_ayrgzK-DcHbQm-9q1O_0wh6_x798z0DZwf-4Sq7-9Pq5eJlxoeVgX0C8EmMvA</recordid><startdate>201612</startdate><enddate>201612</enddate><creator>Voiculescu, M.</creator><creator>Nygrén, T.</creator><creator>Aikio, A. T.</creator><creator>Vanhamäki, H.</creator><creator>Pierrard, V.</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-5014-7682</orcidid><orcidid>https://orcid.org/0000-0002-3454-0350</orcidid><orcidid>https://orcid.org/0000-0002-1864-3878</orcidid><orcidid>https://orcid.org/0000-0001-8838-5125</orcidid></search><sort><creationdate>201612</creationdate><title>Postmidnight ionospheric troughs in summer at high latitudes</title><author>Voiculescu, M. ; Nygrén, T. ; Aikio, A. T. ; Vanhamäki, H. ; Pierrard, V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4670-6211b73c1a4156c4b72c2379434c5ef180f15712fe3d91fc6bcac066117276bd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Convection</topic><topic>Convection heating</topic><topic>Electron energy</topic><topic>Electron precipitation</topic><topic>Electron temperature</topic><topic>Electron temperatures</topic><topic>Evolution</topic><topic>F region</topic><topic>F region trough</topic><topic>Formations</topic><topic>Geophysics</topic><topic>Heating</topic><topic>ion heating</topic><topic>Ion temperature</topic><topic>Ionosphere</topic><topic>ionospheric convection</topic><topic>Latitude</topic><topic>Minima</topic><topic>Plasma</topic><topic>Plasma convection</topic><topic>Plasma density</topic><topic>Plasmas (physics)</topic><topic>Radar</topic><topic>Radar networks</topic><topic>Scattering</topic><topic>Troughs</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Voiculescu, M.</creatorcontrib><creatorcontrib>Nygrén, T.</creatorcontrib><creatorcontrib>Aikio, A. T.</creatorcontrib><creatorcontrib>Vanhamäki, H.</creatorcontrib><creatorcontrib>Pierrard, V.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Voiculescu, M.</au><au>Nygrén, T.</au><au>Aikio, A. T.</au><au>Vanhamäki, H.</au><au>Pierrard, V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Postmidnight ionospheric troughs in summer at high latitudes</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2016-12</date><risdate>2016</risdate><volume>121</volume><issue>12</issue><spage>12,171</spage><epage>12,185</epage><pages>12,171-12,185</pages><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>In this article we identify possible mechanisms for the formation of postmidnight ionospheric troughs during summer, in sunlit plasma. Four events were identified in measurements of European Incoherent Scatter and ESR radars during CP3 experiments, when the ionosphere was scanned in a meridional plan. The spatial and temporal variation of plasma density, ion, and electron temperatures were analyzed for each of the four events. Super Dual Auroral Radar Network plasma velocity measurements were added, when these were available. For all high‐latitude troughs the ion temperatures are high at density minima (within the trough), at places where the convection plasma velocity is eastward and high. There is no significant change in electron temperature inside the trough, regardless of its temporal evolution. We find that troughs in sunlit plasma form in two steps: the trough starts to form when energetic electron precipitation leads to faster recombination in the F region, and it deepens when entering a region with high eastward flow, producing frictional heating and further depleting the plasma. The high‐latitude plasma convection plays an important role in formation and evolution of troughs in the postmidnight sector in sunlit plasma. During one event a second trough is identified at midlatitudes, with different characteristics, which is most likely produced by a rapid subauroral ion drift in the premidnight sector.
Key Points
The high‐latitude plasma convection plays a role in formation and evolution of troughs in the postmidnight sector in sunlit plasma
Ion temperatures are high at density minima (within the trough) at places where the convection plasma velocity is eastward and high
A two‐step process leads to formation of troughs in sunlit plasma: (1) energetic electron precipitation and (2) frictional heating</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2016JA023360</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0001-5014-7682</orcidid><orcidid>https://orcid.org/0000-0002-3454-0350</orcidid><orcidid>https://orcid.org/0000-0002-1864-3878</orcidid><orcidid>https://orcid.org/0000-0001-8838-5125</orcidid></addata></record> |
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subjects | Convection Convection heating Electron energy Electron precipitation Electron temperature Electron temperatures Evolution F region F region trough Formations Geophysics Heating ion heating Ion temperature Ionosphere ionospheric convection Latitude Minima Plasma Plasma convection Plasma density Plasmas (physics) Radar Radar networks Scattering Troughs |
title | Postmidnight ionospheric troughs in summer at high latitudes |
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