A Bottomside Parameterization for the Empirical Canadian High Arctic Ionospheric Model

In this study, we present a bottomside model representation to be used by the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM). This model features a new approach to modeling the bottomside electron density; namely, instead of modelling electron density directly, E‐CHAIM models the altitud...

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Veröffentlicht in:Radio science 2019-05, Vol.54 (5), p.397-414
Hauptverfasser: Themens, David R., Jayachandran, P.T., McCaffrey, Anthony M., Reid, Benjamin, Varney, Roger H.
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container_end_page 414
container_issue 5
container_start_page 397
container_title Radio science
container_volume 54
creator Themens, David R.
Jayachandran, P.T.
McCaffrey, Anthony M.
Reid, Benjamin
Varney, Roger H.
description In this study, we present a bottomside model representation to be used by the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM). This model features a new approach to modeling the bottomside electron density; namely, instead of modelling electron density directly, E‐CHAIM models the altitude profile of the scale thickness of a single bottomside layer. In this approach, the curvature in the bottomside associated with the E region and F1 layer is represented in the scale thickness domain as a peak function centered at the layer peak altitude. The use of this approach ensures the production of explicitly doubly differentiable bottomside electron density profiles and directly avoids issues known to exist within current standards, such as the International Reference Ionosphere (IRI), which has discontinuities in space, time, and in the vertical electron density gradient. In terms of performance, after removing the impacts of hmF2 and NmF2, the new E‐CHAIM profile function generally performs comparably to the IRI, with bottomside TEC from both models within 2.0 TECU (1 TECU = 1016 e/m3) of observations. More specifically, the E‐CHAIM bottomside is demonstrated to outperform the IRI bottomside function in the F region during low solar activity periods with respect to incoherent scatter radar observations. At high latitudes, E‐CHAIM tends to outperform the IRI during winter months by between 10% and 40% of NmF2 while being outperformed by the IRI by between 10% and 25% of NmF2 during summer periods, mainly during the daytime at high solar activity. Key Points A bottomside function for the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM) is presented The IRI demonstrates electron density discontinuities in space, time, and in its vertical gradients The E‐CHAIM bottomside function performs comparably to the IRIs while avoiding the need for discontinuous behavior and ensuring continuous derivatives
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This model features a new approach to modeling the bottomside electron density; namely, instead of modelling electron density directly, E‐CHAIM models the altitude profile of the scale thickness of a single bottomside layer. In this approach, the curvature in the bottomside associated with the E region and F1 layer is represented in the scale thickness domain as a peak function centered at the layer peak altitude. The use of this approach ensures the production of explicitly doubly differentiable bottomside electron density profiles and directly avoids issues known to exist within current standards, such as the International Reference Ionosphere (IRI), which has discontinuities in space, time, and in the vertical electron density gradient. In terms of performance, after removing the impacts of hmF2 and NmF2, the new E‐CHAIM profile function generally performs comparably to the IRI, with bottomside TEC from both models within 2.0 TECU (1 TECU = 1016 e/m3) of observations. More specifically, the E‐CHAIM bottomside is demonstrated to outperform the IRI bottomside function in the F region during low solar activity periods with respect to incoherent scatter radar observations. At high latitudes, E‐CHAIM tends to outperform the IRI during winter months by between 10% and 40% of NmF2 while being outperformed by the IRI by between 10% and 25% of NmF2 during summer periods, mainly during the daytime at high solar activity. Key Points A bottomside function for the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM) is presented The IRI demonstrates electron density discontinuities in space, time, and in its vertical gradients The E‐CHAIM bottomside function performs comparably to the IRIs while avoiding the need for discontinuous behavior and ensuring continuous derivatives</description><identifier>ISSN: 0048-6604</identifier><identifier>EISSN: 1944-799X</identifier><identifier>DOI: 10.1029/2018RS006748</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Altitude ; bottomside ; Curvature ; Density ; E region ; Electron density ; Electron density profiles ; Electrons ; E‐CHAIM, IRI ; F region ; high latitudes ; Incoherent scatter radar ; International standardization ; ionosonde ; Ionosphere ; Parameterization ; Plasma ; Polar environments ; Solar activity ; Thickness</subject><ispartof>Radio science, 2019-05, Vol.54 (5), p.397-414</ispartof><rights>2019. 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This model features a new approach to modeling the bottomside electron density; namely, instead of modelling electron density directly, E‐CHAIM models the altitude profile of the scale thickness of a single bottomside layer. In this approach, the curvature in the bottomside associated with the E region and F1 layer is represented in the scale thickness domain as a peak function centered at the layer peak altitude. The use of this approach ensures the production of explicitly doubly differentiable bottomside electron density profiles and directly avoids issues known to exist within current standards, such as the International Reference Ionosphere (IRI), which has discontinuities in space, time, and in the vertical electron density gradient. In terms of performance, after removing the impacts of hmF2 and NmF2, the new E‐CHAIM profile function generally performs comparably to the IRI, with bottomside TEC from both models within 2.0 TECU (1 TECU = 1016 e/m3) of observations. More specifically, the E‐CHAIM bottomside is demonstrated to outperform the IRI bottomside function in the F region during low solar activity periods with respect to incoherent scatter radar observations. At high latitudes, E‐CHAIM tends to outperform the IRI during winter months by between 10% and 40% of NmF2 while being outperformed by the IRI by between 10% and 25% of NmF2 during summer periods, mainly during the daytime at high solar activity. Key Points A bottomside function for the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM) is presented The IRI demonstrates electron density discontinuities in space, time, and in its vertical gradients The E‐CHAIM bottomside function performs comparably to the IRIs while avoiding the need for discontinuous behavior and ensuring continuous derivatives</description><subject>Altitude</subject><subject>bottomside</subject><subject>Curvature</subject><subject>Density</subject><subject>E region</subject><subject>Electron density</subject><subject>Electron density profiles</subject><subject>Electrons</subject><subject>E‐CHAIM, IRI</subject><subject>F region</subject><subject>high latitudes</subject><subject>Incoherent scatter radar</subject><subject>International standardization</subject><subject>ionosonde</subject><subject>Ionosphere</subject><subject>Parameterization</subject><subject>Plasma</subject><subject>Polar environments</subject><subject>Solar activity</subject><subject>Thickness</subject><issn>0048-6604</issn><issn>1944-799X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp90D1PwzAQBmALgUQpbPwAS6wEzh9x7LGUQisVgVpAbJHjONRVEhc7FSq_nqAyMDHd8rx3pxehcwJXBKi6pkDkYgkgMi4P0IAozpNMqbdDNADgMhEC-DE6iXENQHgq-AC9jvCN7zrfRFda_KSDbmxng_vSnfMtrnzA3criSbNxwRld47Fudel0i6fufYVHwXTO4Jlvfdys-pzBD7609Sk6qnQd7dnvHKKXu8nzeJrMH-9n49E8Mbz_ONGWFClQCywDYVilSKlIYSijIKmxgtqUMlZInqaECKsqpgSRTGSFpGnRJ4boYr93E_zH1sYuX_ttaPuTOaVMZTQVmerV5V6Z4GMMtso3wTU67HIC-U9z-d_mek73_NPVdvevzRe3SwqZpOwbDuZtiA</recordid><startdate>201905</startdate><enddate>201905</enddate><creator>Themens, David R.</creator><creator>Jayachandran, P.T.</creator><creator>McCaffrey, Anthony M.</creator><creator>Reid, Benjamin</creator><creator>Varney, Roger H.</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-2567-8187</orcidid><orcidid>https://orcid.org/0000-0001-5039-7358</orcidid><orcidid>https://orcid.org/0000-0002-5976-2638</orcidid></search><sort><creationdate>201905</creationdate><title>A Bottomside Parameterization for the Empirical Canadian High Arctic Ionospheric Model</title><author>Themens, David R. ; Jayachandran, P.T. ; McCaffrey, Anthony M. ; Reid, Benjamin ; Varney, Roger H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4102-ae1b502e03706c3f91d91bc232082ce62e5233b8455116e9f39618367b825b6c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Altitude</topic><topic>bottomside</topic><topic>Curvature</topic><topic>Density</topic><topic>E region</topic><topic>Electron density</topic><topic>Electron density profiles</topic><topic>Electrons</topic><topic>E‐CHAIM, IRI</topic><topic>F region</topic><topic>high latitudes</topic><topic>Incoherent scatter radar</topic><topic>International standardization</topic><topic>ionosonde</topic><topic>Ionosphere</topic><topic>Parameterization</topic><topic>Plasma</topic><topic>Polar environments</topic><topic>Solar activity</topic><topic>Thickness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Themens, David R.</creatorcontrib><creatorcontrib>Jayachandran, P.T.</creatorcontrib><creatorcontrib>McCaffrey, Anthony M.</creatorcontrib><creatorcontrib>Reid, Benjamin</creatorcontrib><creatorcontrib>Varney, Roger H.</creatorcontrib><collection>CrossRef</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Radio science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Themens, David R.</au><au>Jayachandran, P.T.</au><au>McCaffrey, Anthony M.</au><au>Reid, Benjamin</au><au>Varney, Roger H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Bottomside Parameterization for the Empirical Canadian High Arctic Ionospheric Model</atitle><jtitle>Radio science</jtitle><date>2019-05</date><risdate>2019</risdate><volume>54</volume><issue>5</issue><spage>397</spage><epage>414</epage><pages>397-414</pages><issn>0048-6604</issn><eissn>1944-799X</eissn><abstract>In this study, we present a bottomside model representation to be used by the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM). This model features a new approach to modeling the bottomside electron density; namely, instead of modelling electron density directly, E‐CHAIM models the altitude profile of the scale thickness of a single bottomside layer. In this approach, the curvature in the bottomside associated with the E region and F1 layer is represented in the scale thickness domain as a peak function centered at the layer peak altitude. The use of this approach ensures the production of explicitly doubly differentiable bottomside electron density profiles and directly avoids issues known to exist within current standards, such as the International Reference Ionosphere (IRI), which has discontinuities in space, time, and in the vertical electron density gradient. In terms of performance, after removing the impacts of hmF2 and NmF2, the new E‐CHAIM profile function generally performs comparably to the IRI, with bottomside TEC from both models within 2.0 TECU (1 TECU = 1016 e/m3) of observations. More specifically, the E‐CHAIM bottomside is demonstrated to outperform the IRI bottomside function in the F region during low solar activity periods with respect to incoherent scatter radar observations. At high latitudes, E‐CHAIM tends to outperform the IRI during winter months by between 10% and 40% of NmF2 while being outperformed by the IRI by between 10% and 25% of NmF2 during summer periods, mainly during the daytime at high solar activity. Key Points A bottomside function for the Empirical Canadian High Arctic Ionospheric Model (E‐CHAIM) is presented The IRI demonstrates electron density discontinuities in space, time, and in its vertical gradients The E‐CHAIM bottomside function performs comparably to the IRIs while avoiding the need for discontinuous behavior and ensuring continuous derivatives</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2018RS006748</doi><tpages>18</tpages><orcidid>https://orcid.org/0000-0003-2567-8187</orcidid><orcidid>https://orcid.org/0000-0001-5039-7358</orcidid><orcidid>https://orcid.org/0000-0002-5976-2638</orcidid><oa>free_for_read</oa></addata></record>
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subjects Altitude
bottomside
Curvature
Density
E region
Electron density
Electron density profiles
Electrons
E‐CHAIM, IRI
F region
high latitudes
Incoherent scatter radar
International standardization
ionosonde
Ionosphere
Parameterization
Plasma
Polar environments
Solar activity
Thickness
title A Bottomside Parameterization for the Empirical Canadian High Arctic Ionospheric Model
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