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  <title>Influence of the Stratospheric Quasi-Biennial Oscillation on the Seasonal Variation in the Mesosphere and Lower Thermosphere Based on a Long-Term Reanalysis JAWARA</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/influence-stratospheric-quasi-biennial-oscillation-seasonal-variation</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Influence of the Stratospheric Quasi-Biennial Oscillation on the Seasonal Variation in the Mesosphere and Lower Thermosphere Based on a Long-Term Reanalysis JAWARA&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="2026-01-08T09:43:32-07:00" title="Thursday, January 8, 2026 - 09:43" class="datetime"&gt;Thu, 01/08/2026 - 09:43&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;Jan 8, 2026&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;a href="https://doi.org/10.1175/JAS-D-25-0092.1"&gt;&lt;em&gt;&lt;strong&gt;Journal of the Atmospheric Sciences&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;In the equatorial region, the influence of the stratospheric quasi-biennial oscillation (QBO) extends into the mesosphere and lower thermosphere (MLT) region. This work (&lt;strong&gt;D. Koshin&lt;/strong&gt; and K. Sato) presents the characteristics of this response to the QBO in terms of the semiannual oscillations (SAOs) around the stratopause and the mesopause, and the tides, using the long-term global reanalysis for the whole neutral atmosphere over 19 years of 2004–23. The results indicate that the response is observed at a wide height region of the mesosphere and lower thermosphere, with dominance in two separate height regions, at altitudes around 80 and 100 km. The lower one is observed as a vertical shift of the easterly shear during equinoxes, which can be explained by the difference in the QBO phase-dependent filtering of waves in the stratosphere. The upper one is observed as a stronger easterly during the QBO westerly phase at 10 hPa, in all seasons, associated with larger amplitude and the forcing due to the migrating diurnal tide (DW1). The DW1 propagation latitude region, i.e., the region where the sum of relative and planetary vorticity is equal to or smaller than the frequency of DW1, is relatively wider in the middle mesosphere during the QBO westerly phase. These results suggest that there is a two-step mechanism: first, direct modulation of the upper-mesospheric zonal wind by the QBO through selective wave transmission, and second, the variation in the lower thermospheric zonal wind through selective DW1 transmission due to modulated vorticity.&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/2026-01/Koshin_ZonalWind.png?itok=9jKX4cHa" width="926" height="573" alt="Zonal wind" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Time and height section of the monthly mean zonal-mean zonal wind in the latitudinal range of 108S–108N for (a) climatology, (b) stratosphere quasi biennial oscillation (SQBO) easterly composite, (c) SQBO westerly composite, and (d) the difference (i.e., SQBO easterly2 SQBO westerly). Contour intervals are 10 m s21 and 5 m s21 in (d). (e) The annual mean of the difference and its standard deviation. The results show the QBO in the stratosphere can have significant influence on the mesosphere and lower thermosphere altitudes.&lt;/p&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/influence-stratospheric-quasi-biennial-oscillation-seasonal-variation" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2026-01/Koshin_ZonalWind.png?itok=BWC6QXNo" width="380" height="254" alt="Zonal wind" class="image-style-teaser-380x254 img-fluid"&gt;

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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Jan 8, 2026&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/influence-stratospheric-quasi-biennial-oscillation-seasonal-variation"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Influence of the Stratospheric Quasi-Biennial Oscillation on the Seasonal Variation in the Mesosphere and Lower Thermosphere Based on a Long-Term Reanalysis JAWARA&lt;/span&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;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 href="https://www2.hao.ucar.edu/news/publication-highlight/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Contribution of Gravity Waves to the Lower Thermospheric Winter-to-summer Meridional Circulation in High-resolution WACCM-X&lt;/span&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="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;

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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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 11, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/news-article/new-ai-based-methods-3d-reconstruction-solar-photosphere"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;New AI Based Methods for 3D Reconstruction of the Solar Photosphere&lt;/span&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;

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      &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;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/mhd-simulations-cme-associated-prominence-eruption"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;MHD simulations of CME with associated prominence eruption&lt;/span&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;

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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;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;

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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;
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              &lt;div class="field__item"&gt;&lt;time datetime="2026-01-08T12:00:00Z" class="datetime"&gt;Thu, 01/08/2026 - 12:00&lt;/time&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Thu, 08 Jan 2026 16:43:32 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">1090 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Contribution of Gravity Waves to the Lower Thermospheric Winter-to-summer Meridional Circulation in High-resolution WACCM-X</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Contribution of Gravity Waves to the Lower Thermospheric Winter-to-summer Meridional Circulation in High-resolution WACCM-X&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;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Dec 10, 2025&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;Journal of Geophysical Research, Atmospheres: &amp;nbsp;In the lower thermosphere, there is a large circulation from the winter polar region to the summer polar region at an altitude around 120 km. This study analyzed the role of gravity waves contributing to this circulation using output from a high-resolution simulation. In the winter middle atmosphere, gravity waves with eastward phase speeds are generated around the polar vortex and propagate into the lower thermosphere. Gravity waves are typically assumed to originate in the troposphere and are thought to be unable to propagate above the strong winds in the mesosphere. This study highlights the importance of gravity wave generation in the middle atmosphere and suggests a method for improving parameterized gravity waves. Additionally, the vertical structure of the zonal mean zonal wind is important through the selective filtering of gravity waves. In the summer hemisphere, semidiurnal tidal forcing largely contributes to the lower thermospheric circulation, as do gravity waves. Thus, the lower thermospheric circulation is driven by gravity waves generated in the mesosphere and filtered in the upper mesosphere, as well as by the semidiurnal tide.&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/2025-12/Pedatella_Time-latitude%20sections%20for%20small%20scale%20waves.png?itok=u7oL2DG8" width="926" height="593" alt="Time-latitude sections for small scale waves" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Time-latitude sections of (a) the meridional component of the residual mean circulation and (b) the vertical momentum flux divergence for small scale waves based on high-resolution (0.25 degree) WACCM-X simulations. The results illustrate the role of small scale wave forcing on driving the interhemisphere circulation in the lower thermosphere, including its seasonal variation.&lt;/p&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/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Pedatella_Time-latitude%20sections%20for%20small%20scale%20waves.png?itok=U-Y-HrkZ" width="380" height="254" alt="Time-latitude sections for small scale waves" class="image-style-teaser-380x254 img-fluid"&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/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Rempel_MachineLearningFlowchart.jpg?itok=yPrfXpPu" width="380" height="254" alt="Machine Learning Flowchart" class="image-style-teaser-380x254 img-fluid"&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 href="https://www2.hao.ucar.edu/news/publication-highlight/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Spectropolarimetric Inversion in Four Dimensions with Deep Learning (SPIn4D): II. A Physics-Informed Machine Learning Method for 3D Solar Photosphere Reconstruction&lt;/span&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;

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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;

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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;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;

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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Sep 16, 2025&lt;/div&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;

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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;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;

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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/30" hreflang="en"&gt;Hanli Liu&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/16" hreflang="en"&gt;Nick Pedatella&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Wed, 10 Dec 2025 20:45:29 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">1084 at https://www2.hao.ucar.edu</guid>
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  <title>Local Time Variability of Gravity Wave Activity Revealed by SABER Temperature Observations</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/local-time-variability-gravity-wave-activity-revealed-saber-temperature</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Local Time Variability of Gravity Wave Activity Revealed by SABER Temperature Observations&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="2025-12-10T13:37:23-07:00" title="Wednesday, December 10, 2025 - 13:37" class="datetime"&gt;Wed, 12/10/2025 - 13:37&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;Dec 10, 2025&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;em&gt;&lt;strong&gt;Geophysical Research Letters&lt;/strong&gt;&lt;/em&gt;: &amp;nbsp;We investigate diurnal variability in gravity wave activity, which is an indication of the interaction between gravity waves and tides. We use satellite observations covering almost all solar local times, to estimate the potential energy of gravity waves at each local time. In the equatorial region between 15°S and 15°N, a clear diurnal cycle is observed. This structure is attributed to the static stability associated with the diurnal tide. In the midlatitudes, at 15–60°N and 15–60°S, a semidiurnal variation is observed at altitudes above 90 km. This structure can also be explained by the static stability associated with the semidiurnal tide. These results are generally consistent with previous ground-based observations, although the spatial coverage of ground-based observations is limited. Thus, this study provides a global view of the interaction between gravity waves and tides in the real atmosphere.&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/2025-12/Pedatella_TIMED-SABER%20observations.png?itok=Nlnx-2Ec" width="926" height="682" alt=" TIMED/SABER observations" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Local time-height section of the gravity wave potential energy derived from TIMED/SABER observations. The results are averaged for 50–60°S, 20–30°S, 5°S–5°N, 20–30°N, and 50–60°N (from left to right) for NDJ, FMA, MJJ, and ASO (from top to bottom). These results illustrate the significant local time variation in the gravity wave potential energy, and how it varies with season and latitude.&lt;/p&gt;
          &lt;/figcaption&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;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/quantifying-impact-solar-irradiance-uncertainty-thermosphere-ionosphere"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Quantifying the Impact of Solar Irradiance Uncertainty on Thermosphere-Ionosphere Variability Using Ensemble Forecasts&lt;/span&gt;
&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;
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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;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Contribution of Gravity Waves to the Lower Thermospheric Winter-to-summer Meridional Circulation in High-resolution WACCM-X&lt;/span&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/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Rempel_MachineLearningFlowchart.jpg?itok=yPrfXpPu" width="380" height="254" alt="Machine Learning Flowchart" 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 23, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Spectropolarimetric Inversion in Four Dimensions with Deep Learning (SPIn4D): II. A Physics-Informed Machine Learning Method for 3D Solar Photosphere Reconstruction&lt;/span&gt;
&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/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;
    &lt;a href="https://www2.hao.ucar.edu/news/news-article/nasa-selects-nsf-ncar-heliophysics-mission-continued-development"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;NASA selects NSF NCAR Heliophysics Mission for Continued Development&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&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/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;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/news-article/new-ai-based-methods-3d-reconstruction-solar-photosphere"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;New AI Based Methods for 3D Reconstruction of the Solar Photosphere&lt;/span&gt;
&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/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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Sep 16, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/mhd-simulations-cme-associated-prominence-eruption"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;MHD simulations of CME with associated prominence eruption&lt;/span&gt;
&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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/local-time-variability-gravity-wave-activity-revealed-saber-temperature"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Local Time Variability of Gravity Wave Activity Revealed by SABER Temperature Observations&lt;/span&gt;
&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&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/30" hreflang="en"&gt;Hanli Liu&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/16" hreflang="en"&gt;Nick Pedatella&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Wed, 10 Dec 2025 20:37:23 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">1083 at https://www2.hao.ucar.edu</guid>
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  <title>Quantifying the Impact of Solar Irradiance Uncertainty on Thermosphere-Ionosphere Variability Using Ensemble Forecasts</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/quantifying-impact-solar-irradiance-uncertainty-thermosphere-ionosphere</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Quantifying the Impact of Solar Irradiance Uncertainty on Thermosphere-Ionosphere Variability Using Ensemble Forecasts&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="2025-12-10T11:11:52-07:00" title="Wednesday, December 10, 2025 - 11:11" class="datetime"&gt;Wed, 12/10/2025 - 11:11&lt;/time&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2025-12/Histogram_DEN_SWARM_std_day-Hsu.png?itok=6fXqoJ0p" width="926" height="463" alt="Histogram: dayside Swarm neutral density" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Histogram of the normalized model–data difference (Ai) for dayside Swarm neutral density. The grey histogram shows Ai computed from the WACCM-X ensemble using the new method (EXP 3). The green and red histograms represent Ai computed using the old method (EXP 1 and EXP 2). The blue histogram shows Ai computed with the new method, but with doubled spread (EXP 4). The top row presents the Ai distributions for Swarm-A, and the bottom row shows those for Swarm-C. Blue dashed lines indicate the ±3-standard-deviation thresholds.&lt;/p&gt;
          &lt;/figcaption&gt;
  &lt;/figure&gt;
&lt;p&gt;&lt;a href=" https://doi.org/10.1029/2025SW004612"&gt;&lt;em&gt;&lt;strong&gt;Space Weather&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;This study investigates the sensitivity of the thermosphere and ionosphere to variations in solar spectral irradiance. Using data from the SDO and SORCE missions collected between 2010 and 2018, we quantified the variability and uncertainty of solar spectral irradiance across wavelengths from 0.1 to 190 nm and developed a data-driven method to generate perturbed versions of the irradiance. These perturbations were used to drive ensemble simulation experiments conducted during the 2021/2022 winter to assess sensitivity in the thermosphere and ionosphere. In addition to the experiment using statistically derived perturbations, three more ensemble experiments driven by different perturbation methods were also performed.&lt;br&gt;Results show that both neutral temperature and electron density are highly sensitive to uncertainty in solar spectral irradiance, especially above 200 km altitude. Electron density is particularly influenced by soft X-ray variability in the lower ionosphere. Comparisons with Swarm, ICON, and COSMIC-2 satellite observations confirm the performance of ensemble simulation experiments on capturing the realistic thermospheric and ionospheric variability. Among the experiments, the one driven by statistically derived perturbations produces ensemble spreads that best match the observed variability. This experiment shows good agreement with all three datasets, while the others tend to overestimate or underestimate the variability.&lt;br&gt;This work highlights the importance of accounting for uncertainty in external solar energy input in space weather models and demonstrates the value of data-informed ensemble simulations in improving the accuracy and reliability of thermosphere and ionosphere forecasts.&lt;/p&gt;&lt;/div&gt;
      
      &lt;/div&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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&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;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;/figure&gt;
  
      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Sep 16, 2025&lt;/div&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;Aug 13, 2025&lt;/div&gt;
  
  
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  <pubDate>Wed, 10 Dec 2025 18:11:52 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>The Long-term Trend of Thermospheric Compositions from Whole Atmospheric Simulation and Satellite Observation</title>
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  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;The Long-term Trend of Thermospheric Compositions from Whole Atmospheric Simulation and Satellite Observation&lt;/span&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;a href="https://agupubs.onlinelibrary.wiley.com/doi/10.1029/2025JA034285"&gt;&lt;em&gt;JGR space physics&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;This study examines the long-term trend of column-integrated atomic oxygen to molecular nitrogen ratio, O/N2, in the upper atmosphere and investigates the cause of this long-term trend in O/N2. We first validate the feasibility of using a physics-based model for a long-term climate reanalysis by applying a model-data comparison between 2002 and 2018. O/N2 simulated by NSF NCAR's Whole Atmosphere Community Climate Model with thermosphere and ionosphere extension (WACCM-X) and measured by Global Ultraviolet Imager (GUVI) aboard the Thermosphere Ionosphere Mesosphere Energetics and Dynamics (TIMED) mission is used to determine the long-term trend of O/N2 from 2002 to 2018 and validate the model result. The model and data show good agreement after removing the impact of solar irradiance and geomagnetic activity using a least-squares fitting method, revealing a decreasing trend of O/N2 of about -0.54% per decade relative to the O/N2 in 2018 in the model and about -0.45% per decade in data along the satellite orbit during the period between 2002 and 2018. A decreasing trend of global O/N2 of about -0.70% per decade is found in the model between 1960 and 2018. After that, four WACCM-X long-term simulations are performed from 1960 to 2018 to identify the cause of the decreasing trend of O/N2. The results show that this decreasing trend is mainly caused by the increase in greenhouse gas concentrations.&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/2025-11/on2_data_model.jpg?itok=XcHAVqEl" width="926" height="694" alt="O/N2 measured by TIMED/GUVI and simulated by WACCM-X Case4 and their linear trends" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;O/N2 measured by TIMED/GUVI and simulated by WACCM-X Case4 and their linear trends. (a) Black and grey lines are the O/N2 data derived from TIMED/GUVI and simulated by WACCM-X, respectively. (b) Dark and light green lines are the fitting curves of the black and grey lines in (a) using the least-squares fitting method with an equation that includes the annual, semi-annual, F10.7 index, and Ap index variations. (c) The blue line is the residual term of TIMED/GUVI O/N2 by subtracting the dark green line from the black line, while the cyan line is the residual term of WACCM-X O/N2 by subtracting the light green line from the grey line. (d) Red and magenta lines are the fitting results of blue and cyan lines using the least-squares fitting method with a linear equation, respectively.&lt;/p&gt;
          &lt;/figcaption&gt;
  &lt;/figure&gt;
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  <pubDate>Tue, 11 Nov 2025 20:32:51 +0000</pubDate>
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  <title>Seasonal and Interannual Variation of the Interhemispheric Coupling during the Austral Winter in WACCM6</title>
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  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Seasonal and Interannual Variation of the Interhemispheric Coupling during the Austral Winter in WACCM6&lt;/span&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2025-06/Koshin_interhemisphere%20coupling%20simulated%20by%20WACCM6.jpg?itok=Dkuk_Z8d" width="926" height="1281" alt="interhemisphere coupling simulated by WACCM6" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Results showing the interhemisphere coupling simulated by WACCM6 in July, August, and September. Latitude-height sections of (top) temperature (color) and zonal wind (contour), (middle) temperature (color) and zonal wind (contour) anomaly, and (bottom) stream function of the residual mean circulation composites during cold equatorial stratosphere events averaged over Day = 0 to 4. Results for July (left), August (middle), and September (right) are shown.&lt;/p&gt;
          &lt;/figcaption&gt;
  &lt;/figure&gt;
&lt;p&gt;&lt;a href="https://doi.org/10.1029/2024JD043265"&gt;&lt;em&gt;Journal of Geophysical Research–Atomspheres&lt;/em&gt;:&lt;/a&gt; &amp;nbsp;This paper describes the coupling between the winter stratosphere in the Southern Hemisphere and the northern upper mesosphere as seen in a long-term whole atmosphere model simulation. Characteristics in the winter hemisphere were common for events in July, August, and September. However, there were several differences in the summer hemisphere. First, the modulation of the zonal wind and gravity wave forcing is opposite between the early season (July and August) and the late season (September) due to the difference in the background atmosphere. Second, an interannual variation is observed in the altitude of the warming in the summer polar region, with warmings occurring either above or below 100 km. The warming that appears in the upper mesosphere below 100 km altitude is similar to that in previous studies. On the other hand, the warming that appears in the lower thermosphere above 100 km is explained by an additional mechanism through the modulation of the circulation in the lower thermosphere, which has an opposite direction to that in the mesosphere. This interannual variation is associated with the phase of the intraseasonal oscillation in the equatorial mesosphere and lower thermosphere.&lt;/p&gt;&lt;/div&gt;
      
      &lt;/div&gt;
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          &lt;/div&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/influence-stratospheric-quasi-biennial-oscillation-seasonal-variation" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2026-01/Koshin_ZonalWind.png?itok=BWC6QXNo" width="380" height="254" alt="Zonal wind" 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;Jan 8, 2026&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/quantifying-impact-solar-irradiance-uncertainty-thermosphere-ionosphere" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Histogram_DEN_SWARM_std_day-Hsu.png?itok=71A8Mg41" width="380" height="254" alt="Histogram: dayside Swarm neutral density" class="image-style-teaser-380x254 img-fluid"&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;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;
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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;
  
  
  &lt;h3 class="card-title"&gt;
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  &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;
&lt;/div&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;
  
  
  &lt;/div&gt;
&lt;/div&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&gt;
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      &lt;figure&gt;
      
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&lt;/a&gt;
&lt;/div&gt;
      
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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Sep 16, 2025&lt;/div&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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 10, 2025&lt;/div&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/16" hreflang="en"&gt;Nick Pedatella&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Tue, 24 Jun 2025 18:49:31 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>Impact of increasing greenhouse gases on the ionosphere and thermosphere response to a May 2024-like geomagnetic superstorm</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/impact-increasing-greenhouse-gases-ionosphere-and-thermosphere-response</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Impact of increasing greenhouse gases on the ionosphere and thermosphere response to a May 2024-like geomagnetic superstorm&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="2025-06-24T12:38:29-06:00" title="Tuesday, June 24, 2025 - 12:38" class="datetime"&gt;Tue, 06/24/2025 - 12:38&lt;/time&gt;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Jun 24, 2025&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2025-06/Pedatella_Increasing%20greenhouse%20gases%20impact%20ionosphere%2C%20thermosphere.jpg?itok=3kItnh4y" width="926" height="1090" alt="Impact of increasing greenhouse gases on the ionosphere and thermosphere " class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;CESM(WACCM-X) (a) absolute global mean thermosphere neutral density, (b) storm-time change in global mean thermosphere neutral density, and (c) relative storm-time change in global mean thermosphere neutral density. (d) Geomagnetic Kp index used as forcing in CESM(WACCM-X). The CESM(WACCM-X) neutral density results are at an altitude of 350 km, and the storm-time changes are calculated relative to the average values on May 8-9 in each scenario. The storm is simulated in years 2016, 2040, 2061, and 2084, which have surface CO2 values of 403, 500, 652, and 918 ppmv.&lt;/p&gt;
          &lt;/figcaption&gt;
  &lt;/figure&gt;
&lt;p&gt;&lt;a href=" https://doi.org/10.1029/2025GL116445"&gt;&lt;em&gt;Geophysical Research Letters&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;Geomagnetic storms lead to large changes in the Earth’s upper atmosphere (ionosphere and thermosphere) that can have adverse effects on technological systems, such as GPS positioning and orbits of satellites in low-Earth orbit (200-2000 km). It is now understood that increases in greenhouse gas concentrations result in a decrease in the thermosphere neutral density. This is primarily due to CO2 being a radiative cooler at high altitudes, leading to a reduction in temperatures in the mesosphere and thermosphere, and a contraction of the upper atmosphere. The ionosphere is also impacted by changes in CO2. The present study is focused on understanding how changes in the background state of the upper atmosphere due to increases in CO2 alter the response of the ionosphere and thermosphere to geomagnetic storms. Using a coupled Earth system model that includes an atmospheric component that extends to the ionosphere and thermosphere, the response of the upper atmosphere to a geomagnetic superstorm is simulated for different levels of CO2 concentrations. It is found that increasing levels of CO2 generally result in a weaker response of the ionosphere and thermosphere to geomagnetic storms in absolute terms, while their relative responses enhance at higher CO2 levels.&lt;/p&gt;&lt;/div&gt;
      
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  <pubDate>Tue, 24 Jun 2025 18:38:29 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>Multifluid equations for MHD</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/multifluid-equations-mhd</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Multifluid equations for MHD&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="2025-05-23T09:19:59-06:00" title="Friday, May 23, 2025 - 09:19" class="datetime"&gt;Fri, 05/23/2025 - 09:19&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;May 23, 2025&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;em&gt;&lt;strong&gt;JGR Space Physics&lt;/strong&gt;&lt;/em&gt;: &amp;nbsp;The ionized atoms in near-Earth space, the plasma, consist of a number of species including hydrogen, helium, and oxygen in various states of ionization. Hydrogen is usually the predominant component, but other species can play an important role in the dynamics of space plasmas. Computer simulations of these plasmas, including the effects of the magnetic and electric fields, have been quite successful at describing the near-Earth space. However, in general, they have rarely included any ion species other than hydrogen. This paper describes a multifluid approach that makes it possible to include other ion species assuming the ions are tightly bound to magnetic field lines. In this case, the ions all move together perpendicular to the local magnetic field but are free to move individually along the field direction. This work shows how changes in the magnetic field direction can act to accelerate ions along the field, much like a jai alai ball being thrown with a cesta. The work also shows how plasma waves behave in such a multifluid environment. Finally, the paper presents results of a super-computer simulation of the near-Earth space, modeling the behavior of different plasma fluids and their interactions during a geomagnetic storm.&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/2025-05/MFgam.png?itok=7gJZxQt-" width="926" height="497" alt="multifluid MAGE application" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Overview image of the multifluid MAGE application with a separate fluid for plasma of plasmaspheric origin. All panels are shown in the equatorial plane of the magnetosphere and panels (b-e) correspond to the marked box in panel (a). Shown are: the residual, i.e., non-dipolar component, of the northward magnetic field (a); the density and temperature of fluid~1 (b and c); and the density and temperature of fluid~2 (d and e).&lt;/p&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;

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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/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Fri, 23 May 2025 15:19:59 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">1030 at https://www2.hao.ucar.edu</guid>
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  <title>Evaluating F10.7 and F30 radio fluxes as long-term solar proxies of energy deposition in the thermosphere</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/evaluating-f107-and-f30-radio-fluxes-long-term-solar-proxies-energy</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Evaluating F10.7 and F30 radio fluxes as long-term solar proxies of energy deposition in the thermosphere&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="2025-02-25T09:24:07-07:00" title="Tuesday, February 25, 2025 - 09:24" class="datetime"&gt;Tue, 02/25/2025 - 09:24&lt;/time&gt;
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        &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;Feb 25, 2025&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;a href="https://angeo.copernicus.org/articles/43/175/2025/"&gt;&lt;em&gt;&lt;strong&gt;Annale Geophsicae&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;We use model simulations and observations to examine how well the F10.7 and F30 solar radio fluxes have represented solar forcing in the thermosphere during the last 60 years of weakening solar activity. We found that increased saturation of radio fluxes during the last two extended solar minima leads to an overestimation of solar energy deposition, which manifests as a change in the linear relation between thermospheric parameters and F10.7. On the other hand, the linear relation between thermospheric parameters and F30 remains nearly the same throughout the whole studied period because of a recently found relative increase of F30 with respect to F10.7. This explains the earlier finding that F30 correlates better with several ionospheric and thermospheric parameters than F10.7 during recent decades. We note that continued evaluation is needed to see how well F10.7 and F30 will serve as solar proxies in the future when solar activity may start increasing toward the next grand maximum.&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/2025-02/LiyingQianGraphic.jpg?itok=fZtRBwRf" width="926" height="1103" alt="Averaged mass density" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Averaged mass density at 400 km. Black: mass density derived from satellite drag data; blue: simulated mass density using F10.7 as a solar EUV proxy; red: simulated mass density using F30 &amp;nbsp;as a solar EUV proxy. (b) Solid black: mass density ratio of the simulated density using F10.7 as a solar EUV proxy to the density derived from satellite drag; dotted red line: linear fit to the mass density ratio from 1967–1996; dotted black line: linear fit to the mass density ratio from 1967–2019; blue: daily F10.7 for reference. (c) Same as panel (b) but for the case with the simulated mass density using F30 &amp;nbsp;as a solar EUV proxy.&lt;/p&gt;
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  <pubDate>Tue, 25 Feb 2025 16:24:07 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>The Formation Mechanism of Merged EIA During a Storm on 4 November 2021</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/formation-mechanism-merged-eia-during-storm-4-november-2021</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;The Formation Mechanism of Merged EIA During a Storm on 4 November 2021&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;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Feb 5, 2025&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2025-02/Qian_EIAformation%2Bevolution.png?itok=zGGPzxe-" width="926" height="1147" alt="EIA formation and evolution" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Nmax observed by GOLD (a, b) and NmF2 simulated by WACCM-X (c, d) at 20:10 UT on November 03-04, 2021. The red dotted lines represent the magnetic equator. The black dotted lines represent the 0° longitude. The temporal variations of NmF2 at the 0° longitude (40°S - 40°N latitude) from 9:00 UT and 24:00 UT, simulated by WACCM-X, for November 3rd (e) and 4th (f); The corresponding temporal variations of the peak distance of the South and North EIA crests in (e) and (f), for November 3rd (g) and 4th (h).&lt;/p&gt;
          &lt;/figcaption&gt;
  &lt;/figure&gt;
&lt;p&gt;&lt;a href="DOI:10.1029/2024JA032896"&gt;&lt;em&gt;&lt;strong&gt;JGR-Space Physics&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;In this study, we conduct an in-depth analysis of Whole Atmosphere Community Climate Model-eXtended (WACCM-X) simulations to examine physical mechanisms of the formation and evolution of an equatorial ionization anomaly (EIA) merging phenomenon during a storm on November 4th, 2021. A quantitative analysis reveals that the rapid decay of the EIA crests at their poleward sides at altitudes of ~200-250 km plays a crucial role in the EIA merging during that day. This rapid decay is due to the fast recombination at low altitudes (~200-250 km) as the plasma are transported downward by the westward disturbance dynamo electric field (DDEF) and poleward neutral winds during the storm. The results suggested EIA-merging is not merely northern and southern EIA crests moving together, but it involves a crucial rapid decay of the EIA crests at their poleward sides that descended to low altitudes (rapid recombination, ~200-250 km), driven by regional electric fields and neutral winds. This study plays a crucial role in our understanding of the evolution and formation of the merged EIA on November 4th, 2021 during the storm.&lt;/p&gt;&lt;/div&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/quantifying-impact-solar-irradiance-uncertainty-thermosphere-ionosphere" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Histogram_DEN_SWARM_std_day-Hsu.png?itok=71A8Mg41" width="380" height="254" alt="Histogram: dayside Swarm neutral density" 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 10, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/quantifying-impact-solar-irradiance-uncertainty-thermosphere-ionosphere"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Quantifying the Impact of Solar Irradiance Uncertainty on Thermosphere-Ionosphere Variability Using Ensemble Forecasts&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&gt;
  
  
  &lt;/div&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/polarization-fringes-optical-systems-compendium" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Casini_WavelenghtDependence.png?itok=oDOdxjTI" width="380" height="254" alt="Wavelength dependence" 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 23, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/polarization-fringes-optical-systems-compendium"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Polarization fringes in optical systems: a compendium&lt;/span&gt;
&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/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Pedatella_Time-latitude%20sections%20for%20small%20scale%20waves.png?itok=U-Y-HrkZ" width="380" height="254" alt="Time-latitude sections for small scale waves" class="image-style-teaser-380x254 img-fluid"&gt;

&lt;/a&gt;
&lt;/div&gt;
      
    &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;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/contribution-gravity-waves-lower-thermospheric-winter-summer-meridional"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Contribution of Gravity Waves to the Lower Thermospheric Winter-to-summer Meridional Circulation in High-resolution WACCM-X&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&gt;
  
  
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              &lt;div class="col"&gt;&lt;div class="pb-3 pb-md-0"&gt;
      &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/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii" hreflang="en"&gt;&lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/teaser_380x254/public/2025-12/Rempel_MachineLearningFlowchart.jpg?itok=yPrfXpPu" width="380" height="254" alt="Machine Learning Flowchart" 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 23, 2025&lt;/div&gt;
  
  
  &lt;h3 class="card-title"&gt;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/spectropolarimetric-inversion-four-dimensions-deep-learning-spin4d-ii"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Spectropolarimetric Inversion in Four Dimensions with Deep Learning (SPIn4D): II. A Physics-Informed Machine Learning Method for 3D Solar Photosphere Reconstruction&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&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/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;
&lt;/div&gt;
      
    &lt;/figure&gt;
  
      &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;
    &lt;a href="https://www2.hao.ucar.edu/news/news-article/nasa-selects-nsf-ncar-heliophysics-mission-continued-development"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;NASA selects NSF NCAR Heliophysics Mission for Continued Development&lt;/span&gt;
&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/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;
  
  
  &lt;h3 class="card-title"&gt;
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&lt;/a&gt;
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&lt;/div&gt;
              &lt;div class="col"&gt;&lt;div class="pb-3 pb-md-0"&gt;
      &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/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;
&lt;/div&gt;
      
    &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;
    &lt;a href="https://www2.hao.ucar.edu/news/publication-highlight/mhd-simulations-cme-associated-prominence-eruption"&gt;&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;MHD simulations of CME with associated prominence eruption&lt;/span&gt;
&lt;/a&gt;
  &lt;/h3&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;
&lt;/div&gt;
      
    &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;
  &lt;/h3&gt;
  
  
  &lt;/div&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;
&lt;/div&gt;
      
    &lt;/figure&gt;
  
      &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;
  
  
  &lt;/div&gt;
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              &lt;div class="field__item"&gt;&lt;time datetime="2025-02-05T12:00:00Z" class="datetime"&gt;Wed, 02/05/2025 - 12:00&lt;/time&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/28" hreflang="en"&gt;Joseph McInerney&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/27" hreflang="en"&gt;Liying Qian&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/9" hreflang="en"&gt;Wenbin Wang&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/121" hreflang="en"&gt;Geospace Community Modeling&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Wed, 05 Feb 2025 16:29:40 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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