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    <title>magnetosphere</title>
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  <title> Magnetosphere-ionosphere coupling via prescribed field-aligned current simulated by the TIEGCM</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/magnetosphere-ionosphere-coupling-prescribed-field-aligned-current</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt; Magnetosphere-ionosphere coupling via prescribed field-aligned current simulated by the TIEGCM&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;whawkins&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2022-10-12T13:22:26-06:00" title="Wednesday, October 12, 2022 - 13:22" class="datetime"&gt;Wed, 10/12/2022 - 13:22&lt;/time&gt;
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        &lt;div class="fw-bold fs-6"&gt;Author:&lt;/div&gt;
        &lt;div class="author_created__name fs-6"&gt;whawkins&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Oct 12, 2022&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2022-10/Maute_IntegratedJouleHeating2020.png?itok=Fy6tCfH9" width="926" height="806" alt="Simulations of hemispherically integrated Joule heating [GW] polewardd" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Hemispherically integrated Joule heating [GW] poleward of 50o magnetic latitude based on simulations with a prescibed empirical electric potential model: Weimer-POT (blue), with prescribed electric potential and auroral particle precipitation based on an assimilative method: AMIE-POT (black), and with prescribed field-aligned current: OIM-FAC (red) cases for the northern hemisphere (top) and southern hemisphere (bottom)&lt;/p&gt;

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&lt;p&gt;&lt;strong&gt;A. Maute&lt;/strong&gt;, &lt;strong&gt;A.D. Richmond&lt;/strong&gt;, &lt;strong&gt;G. Lu&lt;/strong&gt;, &lt;strong&gt;D. Knipp&lt;/strong&gt;, Y. Shi, B. Anderson assert that the magnetosphere-ionosphere (MI) coupling is crucial in modeling the thermosphere-ionosphere (TI) response to geomagnetic activity. In general circulation models (GCMs) the MI coupling is typically realized by specifying the ion convection and auroral particle precipitation patterns from e.g., empirical or assimilative models. Assimilative models have the advantage that the ion convection and auroral particle precipitation patterns are mutually consistent and based on available observations. However, assimilating a large set of diverse data requires expert knowledge and is time consuming. Empirical models, on the other hand, are convenient to use, but do not capture all the observed spatial and temporal variations. With the availability of AMPERE data, there is an opportunity for employing field-aligned currents (FAC) in numerical models to represent the MI coupling.&amp;nbsp; In this study, we introduce a new method&amp;nbsp; using observed FAC&amp;nbsp; and solve for the interhemispherically asymmetric electric potential distribution. We compared geomagnetic storm simulations using the new approach and two other often-used methods for specifying MI coupling based on empirical and assimilative high latitude electric potentials. The comparison shows general similarities of the thermosphere-ionosphere storm time response and&amp;nbsp; improved temporal variability of the new method compared to using empirical models, but results also illustrate substantial differences due to our uncertain knowledge about the MI coupling process.&lt;/p&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 23, 2025&lt;/div&gt;
  
  
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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              &lt;div class="field__item"&gt;&lt;time datetime="2022-10-12T12:00:00Z" class="datetime"&gt;Wed, 10/12/2022 - 12:00&lt;/time&gt;
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            &lt;h2 class="p-2 px-md-3"&gt;Tags&lt;/h2&gt;
            &lt;div class="p-2 px-md-3 py-md-3"&gt;
              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/43" hreflang="en"&gt;Art Richmond&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/8" hreflang="en"&gt;Astrid Maute&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/63" hreflang="en"&gt;Delores Knipp&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/34" hreflang="en"&gt;Gang Lu&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/2" hreflang="en"&gt;magnetosphere&lt;/a&gt;        &lt;/div&gt;
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</description>
  <pubDate>Wed, 12 Oct 2022 19:22:26 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">727 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>2022 Space Weather Summer School</title>
  <link>https://www2.hao.ucar.edu/news/news-article/2022-space-weather-summer-school</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;2022 Space Weather Summer School&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;whawkins&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2022-08-30T09:45:48-06:00" title="Tuesday, August 30, 2022 - 09:45" class="datetime"&gt;Tue, 08/30/2022 - 09:45&lt;/time&gt;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Aug 30, 2022&lt;/div&gt;
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            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;&lt;strong&gt;FYI, we will not be holding a&amp;nbsp;Space Weather Summer School in 2023. We hope to resume in 2024.&lt;/strong&gt;&lt;/p&gt;

&lt;p&gt;HAO held the latest in a series of successful Space Weather Summer Schools in Boulder, Colorado during the last 2 weeks of July. This unique educational workshop brought together 31 students mainly from the United States along with two students from abroad. Lecturers included experts in solar physics, solar wind, magnetsophere, and ionosphere-thermosphere in order to provide the students with a comprehensive background of the complete space weather system. In addition to lectures on the physics of the system, students learned from experts at the Space Weather Prediction Center about the challenges in making accurate space weather forecasts. Specialists provided an understanding of how space weather processes turn into impacts in human systems such as the power grid. Each day of the school included a computer-based laboratory exercise that let the students get hands-on experience with the models used to simulate space weather. HAO was pleased to once again provide students with an informative, comprehensive, and well well-appreciated introduction to space weather.&lt;/p&gt;


&lt;figure class="media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2022-08/SWSS2022GroupPhoto.png?itok=j_k2P1-d" width="926" height="678" alt="Students and lecturers assembled together outdoors at the Embassy Suites patio area" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;SWSS 2022 Group Photograph&lt;/p&gt;

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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Jan 8, 2026&lt;/div&gt;
  
  
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&lt;/a&gt;
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              &lt;div class="col"&gt;&lt;div class="pb-3 pb-md-0"&gt;
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 23, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 23, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
  &lt;/h3&gt;
  
  
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/news-article/nasa-selects-nsf-ncar-heliophysics-mission-continued-development" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/CMEx.png?itok=s6Yidhep" width="380" height="254" alt="CMEx explorer mission" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 12, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
  &lt;/h3&gt;
  
  
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/news-article/new-ai-based-methods-3d-reconstruction-solar-photosphere" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/manoa-ifa-sun-ai-2.jpg?itok=iqm0W85i" width="380" height="254" alt="sunspot image" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 11, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/mhd-simulations-cme-associated-prominence-eruption" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-09/Yuhong_magneticFieldLines.png?itok=3GkiY4cg" width="380" height="254" alt="Snapshots of the magnetic field lines &amp;amp; the synthetic SDO/AIA 304 Å images" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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    &lt;/figure&gt;
  
      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Sep 16, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
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              &lt;div class="col"&gt;&lt;div class="pb-3 pb-md-0"&gt;
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/local-time-variability-gravity-wave-activity-revealed-saber-temperature" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Pedatella_TIMED-SABER%20observations.png?itok=ETj3ncLi" width="380" height="254" alt=" TIMED/SABER observations" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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    &lt;/figure&gt;
  
      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
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      &lt;figure&gt;
      
            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/efficiency-electromagnetic-energy-transfer-solar-wind-ionosphere-through" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-08/Lin_Electromag%20Energy%20Transfer_Spar.png?itok=7mEsFWr4" width="380" height="254" alt="Electromagnetic Energy Transfer" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/efficiency-electromagnetic-energy-transfer-solar-wind-ionosphere-through"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Efficiency of Electromagnetic Energy Transfer from Solar Wind to Ionosphere through Magnetospheric Ultra-Low Frequency Waves&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&gt;
  
  
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/104" hreflang="en"&gt;Michael Wiltberger&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/29" hreflang="en"&gt;Stan Solomon&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/2" hreflang="en"&gt;magnetosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/5" hreflang="en"&gt;solar wind&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/62" hreflang="en"&gt;space weather&lt;/a&gt;        &lt;/div&gt;
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</description>
  <pubDate>Tue, 30 Aug 2022 15:45:48 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">684 at https://www2.hao.ucar.edu</guid>
    </item>
<item>
  <title>Impacts of binning methods on high-latitude electrodynamic forcing: static vs boundary oriented binning methods</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/impacts-binning-methods-high-latitude-electrodynamic-forcing-static-vs</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Impacts of binning methods on high-latitude electrodynamic forcing: static vs boundary oriented binning methods&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;kolinski&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2021-11-18T11:45:53-07:00" title="Thursday, November 18, 2021 - 11:45" class="datetime"&gt;Thu, 11/18/2021 - 11:45&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: JGR Space Physics; First HAO Author's Name: Art Richmond&lt;/p&gt;

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        &lt;div class="fw-bold fs-6"&gt;Author:&lt;/div&gt;
        &lt;div class="author_created__name fs-6"&gt;kolinski&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Nov 18, 2021&lt;/div&gt;
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            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;The Earth’s atmosphere is coupled at high latitude to the magnetosphere. This is a crucial region since energy is put into the upper atmosphere of Earth and is redistributed globally. Numerical models such as general circulation models (GCMs) simulate the effects of the high latitude energy input on the thermosphere-ionosphere system.&lt;/p&gt;


&lt;figure class="align-left media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2021-11/Richmond_JouleHeating.jpg?itok=d4kuxNFA" width="926" height="437" alt="Distributions of height-integrated Joule heating" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Distributions of height-integrated Joule heating in the northern hemisphere (geographic coordinates) from two GITM simulations for 2002 September 23 0010 UT: (a) Run 1 with static boundary binning and (b) Run 2 with boundary oriented binning. The hemispherically integrated Joule heating is given at the lower left of each plot. There is an 18% increase in integrated heating when employing the boundary oriented binning method.&lt;/p&gt;

          &lt;/figcaption&gt;
  &lt;/figure&gt;


&lt;p&gt;However, an outstanding issue in the GCM simulations for Earth’s upper atmosphere is the inaccurate estimation of energy input, especially the Joule heating, which is associated with the inaccuracy of empirical models for high-latitude electrodynamic forcing. Several factors can contribute to the inaccuracy. In this study, we examine the influence of the binning methods used in the development of those empirical models on the Joule heating. Traditionally, data under similar conditions are binned through a static binning approach by using fixed geomagnetic coordinates, in which the dynamic nature of the forcing is not taken into account and therefore the forcing patterns may be significantly smoothed. To avoid the smoothing issue, data can be binned according to some physically important boundaries in the high-latitude forcing, i.e., through a boundary-oriented binning approach. In this study, we have investigated the sensitivity of high-latitude forcing patterns to the binning methods by applying both static and boundary-oriented binning approaches to the electron precipitation and electric potential data from the Defense Meteorological Satellite Program (DMSP) satellites. The forcing patterns obtained from both static and boundary-oriented binning approaches are used to drive Global Ionosphere and Thermosphere Model (GITM) to assess the impacts on Joule heating by using different binning patterns. It is found that the hemispheric-integrated Joule heating in the simulation driven by the boundary oriented binning patterns is 18% higher than that driven by the static binning patterns for southward IMF dominated case.&lt;/p&gt;
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&lt;/a&gt;
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&lt;/a&gt;
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/efficiency-electromagnetic-energy-transfer-solar-wind-ionosphere-through" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-08/Lin_Electromag%20Energy%20Transfer_Spar.png?itok=7mEsFWr4" width="380" height="254" alt="Electromagnetic Energy Transfer" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/43" hreflang="en"&gt;Art Richmond&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/7" hreflang="en"&gt;Earth's upper atmosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/2" hreflang="en"&gt;magnetosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/13" hreflang="en"&gt;modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Thu, 18 Nov 2021 18:45:53 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">77 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Simulated trends in ionosphere-thermosphere climate due to predicted main magnetic field changes from 2015 to 2065</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/simulated-trends-ionosphere-thermosphere-climate-due-predicted-main</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Simulated trends in ionosphere-thermosphere climate due to predicted main magnetic field changes from 2015 to 2065&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;kolinski&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2021-11-17T12:59:01-07:00" title="Wednesday, November 17, 2021 - 12:59" class="datetime"&gt;Wed, 11/17/2021 - 12:59&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: JGR Space Physics; First HAO Author's Name: Astrid Maute&lt;/p&gt;

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        &lt;div class="fw-bold fs-6"&gt;Author:&lt;/div&gt;
        &lt;div class="author_created__name fs-6"&gt;kolinski&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Nov 17, 2021&lt;/div&gt;
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            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;The strength and structure of the Earth's magnetic field is gradually changing. These changes do not only affect the difference between the geographic and magnetic pole, which we have to consider when we hike in higher latitude regions. The upper atmosphere also reacts to these changes, since the plasma distribution in the upper atmosphere is strongly influenced by Earth's magnetic field, and can feed back to the neutral atmosphere through ion-neutral coupling. With our increasing number of space assets and reliance an them, it is important to understand the space environment changes the Earth's magnetic field will introduce.&lt;/p&gt;


&lt;figure class="align-left media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2021-11/TEC_in2015.jpg?itok=xYxbBzXt" width="926" height="290" alt="TEC plot" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;TEC [TECU] in 2015 (left) and the difference between 2065 and 2015 (right) at 18 UT averaged over all days of the year. The black triangle marks the location of Jicamarca.&lt;/p&gt;

          &lt;/figcaption&gt;
  &lt;/figure&gt;


&lt;p&gt;In this study will we use a predictive model of the Earth's magnetic field together with the Thermosphere-Ionosphere-Electrodynamics General Circulation Model to provide some guidance about the expected upper atmosphere changes from 2015 and year 2065. In general, during the next 50 years the dipole moment is predicted to decrease, with the South Atlantic Anomaly expanding, deepening, and continuing to move westward, while the magnetic dip poles move north-westward. The global mean neutral density in the thermosphere is expected to increase slightly, by up to 1% on average, or up to 2% during geomagnetically disturbed conditions (Kp &amp;gt;= 4). These density trends are small compared to other trend drivers. Global mean changes in total electron content (TEC) range from -3% to +4%, depending on season and UT. However, regional changes can be much larger, up to about +/-35% in the region of ~45deg S-45deg N and 110deg W-0 deg W during daytime. Changes in the vertical ExB drift are the most important driver of changes in TEC, although other plasma transport processes also play a role. A reduction in the low-latitude upward ExB drift weakens the equatorial ionization anomaly in the longitude sector of ~105deg W-60deg W, manifesting itself as a local increase in electron density over Jicamarca (12.0deg S, 76.9deg W). The predicted changes in TEC could make a signifcant contribution to observationally detectable trends.&lt;/p&gt;
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  <pubDate>Wed, 17 Nov 2021 19:59:01 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">65 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Convolutional Neural Networks for Predicting the strength of the Near-Earth Magnetic Field Caused by Interplanetary Coronal Mass Ejections</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/convolutional-neural-networks-predicting-strength-near-earth-magnetic</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Convolutional Neural Networks for Predicting the strength of the Near-Earth Magnetic Field Caused by Interplanetary Coronal Mass Ejections&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;kolinski&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2021-11-17T09:26:43-07:00" title="Wednesday, November 17, 2021 - 09:26" class="datetime"&gt;Wed, 11/17/2021 - 09:26&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: Frontiers in Astronomy; Authors names as they are listed in article: Anna Malanushenko, Natasha Flyer, Sarah Gibson&lt;/p&gt;

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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Nov 17, 2021&lt;/div&gt;
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            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;In this paper, regression-based deep convolutional neural networks (CNN), with 12 layers, are developed for predicting the maximal amplitude of the southward component of the near-Earth magnetic field from a passing interplanetary coronal mass ejection (ICME). The input to the CNN is the Gibson and Low (GLOW) flux rope model (Gibson and Low, 1998) that describes the coronal properties of a CME, where its morphology and position is controlled by 5 varying parameters, i.e. input sampling occurs over a 5D parameter space. The ultimate goal is to determine the extent to which coronal spectropolarimetric observations at the Sun encode sufficient information to predict southward magnetic field component at the Earth.&lt;/p&gt;


&lt;figure class="align-left media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2021-11/AnnaM_FluxRope.png?itok=iTjTLJVE" width="926" height="620" alt="Examples of various initial GLOW configurations" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Examples of various initial GLOW configurations. Blue and green lines are magnetic field lines sampling the magnetic structure of the GLOW spheromak, shown here with different combinations of parameters for angular size, topology, orientation. Solar surface is shown in thin black lines for reference.&lt;/p&gt;

          &lt;/figcaption&gt;
  &lt;/figure&gt;


&lt;p&gt;The GLOW model is used as a first simple test of a self-similarly expanding magnetic flux rope which nevertheless allows consideration of the impact of varying CME location, orientation, size, and morphology. The CNN problem is set up in two experiments: 1) given input data near the Sun, three 2D images in the meridional plane of the components of the magnetic field, predict the maximal southward amplitude of the measured magnetic field at the Earth; 2) given line-of-sight integrated images of the Stokes parameters, corresponding to the physical configurations of the over 30K flux ropes from Part 1, predict the maximal southward amplitude of the measured magnetic field at the Earth.&lt;/p&gt;
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 12, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 11, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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&lt;/a&gt;
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&lt;/a&gt;
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            &lt;div class="field field--name-field-primary-image field--type-entity-reference field--label-hidden field__item"&gt;  &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/efficiency-electromagnetic-energy-transfer-solar-wind-ionosphere-through" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-08/Lin_Electromag%20Energy%20Transfer_Spar.png?itok=7mEsFWr4" width="380" height="254" alt="Electromagnetic Energy Transfer" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
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              &lt;div class="field__item"&gt;&lt;time datetime="2020-07-09T12:00:00Z" class="datetime"&gt;Thu, 07/09/2020 - 12:00&lt;/time&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/54" hreflang="en"&gt;Anna Malanushenko&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/55" hreflang="en"&gt;CME&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/53" hreflang="en"&gt;GLOW&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/2" hreflang="en"&gt;magnetosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/13" hreflang="en"&gt;modeling&lt;/a&gt;        &lt;/div&gt;
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