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    <title>Scott McIntosh</title>
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  <title>A Magnetohydrodynamic Mechanism for the Formation of Solar Polar Vortices</title>
  <link>https://www2.hao.ucar.edu/news/news-article/magnetohydrodynamic-mechanism-formation-solar-polar-vortices</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;A Magnetohydrodynamic Mechanism for the Formation of Solar Polar Vortices&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="2024-11-13T09:03:34-07:00" title="Wednesday, November 13, 2024 - 09:03" class="datetime"&gt;Wed, 11/13/2024 - 09:03&lt;/time&gt;
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          &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/23"&gt;Scott McIntosh&lt;/a&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;Nov 13, 2024&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/10.1073/pnas.2415157121"&gt;&lt;em&gt;&lt;strong&gt;PNAS (Proceedings of National Academy of Sciences)&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: &amp;nbsp;Polar vortices are ubiquitous features of planetary atmospheric flows, from the Earth-like rocky planets to Jupiter- and Saturn-like gas giant planets. Very little is known about their existence or dynamics on the Sun. What should be expected near the Sun’s pole for the upcoming solar multi-viewpoint and polar missions? Here we report the first magnetohydrodynamic nonlinear simulations for the formation and evolution of solar polar vortices using a near-surface magnetohydrodynamic shallow-water model. Our findings indicate that the rush-to-the-poles, the migration of magnetic fields towards the pole following the Sun’s magnetic cycle, can positively contribute to the formation of polar vortices. The mechanism proposed here for the formation of polar vortices is the first one to involve the role of magnetic fields and may be relevant to any star with a magnetic cycle. The Sun’s polar vortices resulting from this mechanism are predominantly magnetohydrodynamic, consisting of a tight pair of cyclonic and anticyclonic swirls. This mechanism is likely to operate during all solar cycle phases except the peak, when the polar field reverses. Polar vortices can impact dynamical evolution of global flows and polar fields, which seed the next activity cycle, hence better knowledge of physics of polar regions may lead to improved solar cycle and space weather forecasts. See: &lt;a href="https://news.ucar.edu/132996/swirling-polar-vortices-likely-exist-sun-new-research-finds"&gt;&lt;em&gt;NSF-NCAR news website&lt;/em&gt;&lt;/a&gt;.&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/2024-11/Dikpati_Evolving_polar_vortex.png?itok=FGf2JspZ" width="926" height="486" alt="Simulation of an evolving polar vortex" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Simulations of magnetohydrodynamically governed polar vortices for a 30-degree inclined view (left) and for a polar view (right). Magnetohydrodynamic simulations show that the initial mid-latitude perturbations tend to drift and cluster around the forming multiple complex cyclonic and anticyclonic swirls. Following the polar rush, these swirls ultimately lead to an evolved configuration consisting of a pair of tight swirls with m=1 pattern.&lt;/p&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, 13 Nov 2024 16:03:34 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">987 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Evolution Of Amplitude And Longitude Phase Of Tachocline Rossby Waves Diffusing To The Photosphere</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/evolution-amplitude-and-longitude-phase-tachocline-rossby-waves</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Evolution Of Amplitude And Longitude Phase Of Tachocline Rossby Waves Diffusing To The Photosphere&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="2024-10-29T13:38:58-06:00" title="Tuesday, October 29, 2024 - 13:38" class="datetime"&gt;Tue, 10/29/2024 - 13:38&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 29, 2024&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/10.1093/mnras/stae2457"&gt;&lt;em&gt;&lt;strong&gt;MNRAS&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;&lt;em&gt;— (Published: 05 November 2024)&lt;/em&gt; &amp;nbsp;Physics of MHD Rossby waves in the tachocline-layer were studied by Dikpati, Gilman, Chatterjee et al. (2020) using a fluid-particle-trajectory approach along with solving vorticity and induction equations. By extending the 2020 MHD Rossby wave model to include a hydrodynamic turbulent convection zone (CZ), they were able to examine how MHD Rossby waves generated in the tachocline might diffuse upward through the CZ to the solar surface. Major findings from this current study include (i) pure hydrodynamic Rossby wave amplitudes decline with height due to viscous diffusion at a rate that is independent of viscosity and increases with longitude wavenumber, (ii) fast MHD Rossby waves amplitude declines faster with height for increasing toroidal field, due to their longitude-phase shifting with height, which increases dissipation of kinetic energy in the wave velocities, (iii) slow MHD Rossby waves decline even faster with height because their longitude-phase shifts more rapidly with height, due to their slow phase speed. Furthermore, it was also found that low wavenumber HD and fast MHD Rossby waves, originating in the tachocline, might be detected at the photosphere, but slow MHD Rossby waves should be virtually impossible to detect. An inference from fluid particle trajectories that wave amplitudes declining with height and longitude phase shifting with height associated with decline, implies a powerful mechanism for tangling of magnetic fields, distinct from convective turbulence effects.&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/2024-10/Dikpati_RW-penetration.png?itok=pLLrv3pr" width="926" height="568" alt="Rosby Wave penetration" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Amplitude decline with height of fast and slow MHD Rossby waves at the top of the channel, centered at 45 degrees latitude, compared to the bottom as a function of toroidal field strength, in kiloGauss, for longitudinal wave numbers m = 1 − 10. Left frame: fast waves; right frame: slow waves. Waves for which amplitude at top is smaller than 10−5 compared to the bottom are not plotted. Amplitude decline with height of the zero kG slow wave is included as a limiting case, even though it does not actually exist in that limit. In the limit of zero toroidal field, the fast wave becomes the hydrodynamic Rossby wave.&lt;/p&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/21" hreflang="en"&gt;Mausumi Dikpati&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/24" hreflang="en"&gt;Peter Gilman&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/23" hreflang="en"&gt;Scott McIntosh&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/116" hreflang="en"&gt;Solar Flux Origins, Emergence, and Eruptions&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Tue, 29 Oct 2024 19:38:58 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">981 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Global and Local Dynamics of X-flare Producing Active Regions During Solar Cycle 25 Peak-Phase</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/global-and-local-dynamics-x-flare-producing-active-regions-during-solar</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Global and Local Dynamics of X-flare Producing Active Regions During Solar Cycle 25 Peak-Phase&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__name fs-6"&gt;whawkins&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Sep 6, 2024&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/10.1051/0004-6361/202451428"&gt;&lt;em&gt;&lt;strong&gt;Astronomy &amp;amp; Astrophysics&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;: As solar cycle (SC) 25 approaches its peak, a number of significant (X-class) flares have been produced. Here, we investigate the circumstances under which two of the most flare-prolific active regions of solar cycle 25, namely ARs 13590 and 13514, flared. Two aspects of the evolution of these active regions are investigated: the global-scale magnetic toroid configuration and small-scale magnetic field morphology and topology, prior, during and after the onset of major flares.&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/2024-09/Ralphaldini_21st%20February%202024%20synopticMap.png?itok=ycHBPkbu" width="926" height="341" alt="21st February 2024 synoptic map" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;All active regions numbered by NOAA are spotted and marked on 21st February 2024 synoptic map constructed from SDO/HMI daily fits files. The double-arrowed top bar indicates which active regions are on the front side. Here, active regions resulting in X-class Flares are highlighted in red, while active regions resulting in M-class flares are highlighted in orange. Blue and red curves represent, respectively, the Northern and Southern Hemisphere magnetic toroid.&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;

&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;
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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;
  
  
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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;
  
  
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  <pubDate>Fri, 06 Sep 2024 16:54:25 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">974 at https://www2.hao.ucar.edu</guid>
    </item>
<item>
  <title>HMI Science Nuggets features: Rossby waves and the organization of photospheric magnetic fields</title>
  <link>https://www2.hao.ucar.edu/news/news-article/hmi-science-nuggets-features-rossby-waves-and-organization-photospheric-magnetic</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;HMI Science Nuggets features: Rossby waves and the organization of photospheric magnetic fields&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="2023-10-06T13:06:26-06:00" title="Friday, October 6, 2023 - 13:06" class="datetime"&gt;Fri, 10/06/2023 - 13:06&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 6, 2023&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2023-05/Raphaldini_Butterfly.png?itok=a_oNzC-N" width="926" height="491" alt="Butterfly diagram" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Comparison of the butterfly diagram based on the Shannon Entropy (top) and the butterfly diagram based on the Magnetic Field Strength (bottom), showing the evolution of level of longitudinal organization of the photospheric magnetic fields as a function of latitude and time.&lt;/p&gt;

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


&lt;p&gt;&lt;a href="http://hmi.stanford.edu/hminuggets/?p=4145"&gt;&lt;em&gt;&lt;strong&gt;HMI Science Nuggets&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;:&amp;nbsp; In recent years an increasing amount of evidence points to the crucial role of magnetically-modified Rossby waves in several solar phenomena. Rossby waves are large scale vortical oscillations that arise in rotating fluid/plasma systems as a result of the Coriolis force, being one of the most fundamental physical mechanisms in the understanding of Earths’s climate and weather. In Earth’s atmosphere one of their effects is to organize the spatial temporal formation of clouds and consequently rainfall and storms. Rays (paths) along which Rossby waves propagate are the origin of atmospheric stormtracks and teleconnection patterns.&lt;/p&gt;
&lt;/div&gt;
      
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&lt;/a&gt;
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&lt;/a&gt;
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  <pubDate>Fri, 06 Oct 2023 19:06:26 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>Deciphering Pre-solar-storm Features Of September-2017 Storm From Global And Local Dynamics</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/deciphering-pre-solar-storm-features-september-2017-storm-global-and</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Deciphering Pre-solar-storm Features Of September-2017 Storm From Global And Local Dynamics&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="2023-08-01T12:47:28-06:00" title="Tuesday, August 1, 2023 - 12:47" class="datetime"&gt;Tue, 08/01/2023 - 12:47&lt;/time&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2023-08/Raphaldini_AR12673FIELDS.png?itok=9Ev39ujy" width="926" height="1232" alt="Evolution of the magnetic fields (left) and helicity density (right) for AR 12673" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Evolution of the magnetic fields (left) and helicity density (right) for AR 12673.&lt;/p&gt;

          &lt;/figcaption&gt;
  &lt;/figure&gt;
&lt;p&gt;We investigate how global toroid patterns and local magnetic field topology of solar active region AR12673 together can hindcast occurrence of the biggest X-flare of cycle 24. Magnetic toroid patterns (narrow latitude-belts warped in longitude, in which active regions are tightly stringed) derived from surface distribution of active regions, prior/during AR12673 emergence, reveal that the portions of South-toroid containing AR12673 was not tipped-away from its North-toroid counterpart at that longitude, unlike the 2003 Halloween storms scenario. During minimum-phase there were too few emergences to determine multi-mode warped toroid patterns in longitude. A new emergence within AR12673 produced a complex/non-potential structure, which led to rapid build-up of helicity and winding that triggered the biggest X-flare of cycle 24. Such a minimum-phase storm can be forecast with only hours' lead-time. However, global patterns and local dynamics for a peak-phase storm, such as that from AR11263, behaved like 2003 Halloween storms, producing the second biggest X-flare of cycle 24. AR11263 was present at the longitude where the North and South toroids tipped-away from each other. Both toroids were warped in longitude due to higher wave numbers and were slowly evolving. While global toroid patterns indicate that pre-storm features can be forecast with a lead-time of a few Carrington Rotations, observed complex/non-potential field structure development hours before the storm can improve the forecast further. We infer that minimum-phase storms can be forecast only hours ahead, while flare-prone active regions in peak-phase can be anticipated at least a month ahead from global toroid patterns.&lt;/p&gt;&lt;/div&gt;
      
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  <pubDate>Tue, 01 Aug 2023 18:47:28 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
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  <title>Analyzing longitude distribution of photospheric magnetic fields from MDI/HMI synoptic maps by using information theory</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/analyzing-longitude-distribution-photospheric-magnetic-fields-mdihmi</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Analyzing longitude distribution of photospheric magnetic fields from MDI/HMI synoptic maps by using information theory&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;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Evidence for Rossby waves&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;whawkins&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;May 18, 2023&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;&lt;em&gt;The Astrophysical Journal&lt;/em&gt;&lt;/strong&gt;:&amp;nbsp; Much of the research on the magnetic activity of the Sun has been focused on its asymmetric component, however the longitudinal complexity plays a fundamental role in the solar magnetic activity. Rossby waves have recently been proposed as a fundamental mechanism regarding the non-asymmetric of the solar magnetic fields. Here, we use HMI and MDI magnetic field synoptic maps to evaluate the magnetic field structures (mainly active regions) organization and propagation as a function of time and latitude. We first demonstrate using information theory that the organization of longitudinal structures observed on synopitc maps is proportional to the level of activity at a given latitude. We further show that this organization on the longitudinal structures is persisent and due to long-lived features. The drift velocity of these long lived photospheric features is inferred, and is shown to significantly vary with latitude and is compatible with the phase speed of tachocline magnetic-Rossby waves with a toroidal field in the range of 5-10 kG. Our results suggest that Rossby waves contribute to the organization and propagation of photospheric magnetic features on the timescale of several months and beyond.&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/2023-05/Raphaldini_Butterfly.png?itok=a_oNzC-N" width="926" height="491" alt="Butterfly diagram" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Comparison of the butterfly diagram based on the Shannon Entropy (top) and the butterfly diagram based on the Magnetic Field Strength (bottom), showing the evolution of level of longitudinal organization of the photospheric magnetic fields as a function of latitude and time.&lt;/p&gt;

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

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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/21" hreflang="en"&gt;Mausumi Dikpati&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/23" hreflang="en"&gt;Scott McIntosh&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Thu, 18 May 2023 19:58:20 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">829 at https://www2.hao.ucar.edu</guid>
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  <title>Magnetohydrodynamics Instabilities of Double Magnetic Bands in a Shallow-water Tachocline Model: I Cross-equatorial Interactions of Bands</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/magnetohydrodynamics-instabilities-double-magnetic-bands-shallow-water</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Magnetohydrodynamics Instabilities of Double Magnetic Bands in a Shallow-water Tachocline Model: I Cross-equatorial Interactions of Bands&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="2023-01-19T15:16:14-07:00" title="Thursday, January 19, 2023 - 15:16" class="datetime"&gt;Thu, 01/19/2023 - 15:16&lt;/time&gt;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Jan 19, 2023&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2023-01/Dikpati_double_band_MHD_instability.png?itok=QA7ALpSW" width="926" height="1309" alt="Double band MHD instability" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;For low effectiive gravity (G = 0.5) growth rate contours for m = 1 modes are displayed in the field-strength space, in which x-axis denotes the strength of the high-latitude band and the y-axis that of the low-latitude band. Left and right panels are respectively for antisymmetric (m = 1,A) and symmetric (m = 1,S) modes. As the band-system migrates from high latitudes towards the equator, four rows from top to the bottom show how the instability features change respectively for bands at 60◦ − 30◦ (aa,ab), 50◦ − 20◦ (ba,bb), 40◦ − 10◦ (ca,cb) and 35◦ − 5◦.&lt;/p&gt;

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


&lt;p&gt;&lt;em&gt;Astrophysical Journal&lt;/em&gt;:&amp;nbsp; Along with the ”butterfly diagram” of sunspots, combined observational studies of ephemeral active regions, X-ray and EUV brightpoints, plage, filaments, faculae and prominences demonstrate a pattern, which is known as the Extended Solar Cycle (ESC). This pattern indicates the wings of the sunspot butterfly could be extended to much higher latitudes (up to ∼ 60 degrees), to earlier time than the start of a sunspot cycle, hence yielding a strong overlap between cycles. Thus during the ongoing cycle’s activity near 30-degrees latitude in each hemisphere, the next cycle kicks off at around 60- degrees. By representing these epochs of overlaps by oppositely-directed double magnetic bands in each hemisphere, we compute the unstable eigenmodes for MHD Rossby waves at the base of the convection zone and study how the properties of these energetically active Rossby waves change as these band-pairs migrate equatorward. We find that in each hemisphere the low-latitude band interacts with the high-latitude band and drive the MHD instability as the solar activity progresses from 35◦ to 15◦ latitude, which is essentially the rising phase. When the activity proceeds further equatorward from 15-degrees, interaction between low- and high-latitude bands weakens, and the cross-equatorial interaction between two low-latitude bands in each hemisphere starts. The eigenmodes in latitude- longitude planforms also reflect such changes in their pattern as the bend of the the active cycle moves below 15-degree latitude.&lt;/p&gt;
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  <pubDate>Thu, 19 Jan 2023 22:16:14 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">782 at https://www2.hao.ucar.edu</guid>
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  <title>Simulating Solar Near-surface Rossby Waves By Inverse-cascade From Supergranule Energy</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/simulating-solar-near-surface-rossby-waves-inverse-cascade-supergranule</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Simulating Solar Near-surface Rossby Waves By Inverse-cascade From Supergranule Energy&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="2022-10-26T12:19:17-06:00" title="Wednesday, October 26, 2022 - 12:19" class="datetime"&gt;Wed, 10/26/2022 - 12:19&lt;/time&gt;
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                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Oct 26, 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;em&gt;Astrophysical Journal—&lt;strong&gt;M. Dikpati&lt;/strong&gt;,&amp;nbsp;&lt;strong&gt;P. A. Gilman&lt;/strong&gt;, G. A. Guerrero, A. G. Kosovichev, &lt;strong&gt;S. W. McIntosh&lt;/strong&gt;, K. R. Sreenivasan, J. Warnecke, T. V. Zaqarashvili&lt;/em&gt;&lt;/p&gt;


&lt;figure class="align-right 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/2022-10/Dikpati_RossbyWaves_from_supergranules_energy.png?itok=18Vx_Kag" width="926" height="2363" alt="Rossby Waves from super granules energy" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Three snapshots during evolution of kinetic energy spectra in spectral space, for initial solid rotation, in a T42 model.&amp;nbsp;&lt;/p&gt;

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


&lt;p&gt;Rossby waves are found at several levels in the Sun, most recently in its supergranule layer. We show that Rossby waves in the supergranule layer can be excited by an inverse cascade of kinetic energy from the nearly horizontal motions in supergranules. We illustrate how this excitation occurs using a hydrodynamic shallow-water model for a 3D thin rotating spherical shell. We find that initial kinetic energy at small spatial scales inverse-cascades quickly to global scales, exciting Rossby waves whose phase velocities are similar to linear Rossby waves on the sphere originally derived by Haurwitz. Modest departures from the Haurwitz formula originate from nonlinear finite amplitude effects and/or the presence of differential rotation. Like supergranules, the initial small scale motions in our model contain very&lt;br&gt;
little vorticity compared to their horizontal divergence, but the resulting Rossby waves are almost all vortical motions. Supergranule kinetic energy could have gone mainly into gravity waves, but we find that most energy inverse-cascades to global Rossby waves. Since kinetic energy in supergranules is three or four orders of magnitude larger than that of the observed Rossby waves in the supergranule layer, there is plenty of energy available to drive the inverse-cascade mechanism. Tachocline Rossby waves were previously shown to play crucial roles in causing "seasons" of space weather through their nonlinear interactions with global flows and magnetic fields. We discuss briefly how various Rossby waves in tachocline, convection zone, supergranule layer and corona can be reconciled in a unified framework.&lt;/p&gt;
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  <pubDate>Wed, 26 Oct 2022 18:19:17 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">747 at https://www2.hao.ucar.edu</guid>
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  <title>Global Maps of the Magnetic Field in the Solar Corona</title>
  <link>https://www2.hao.ucar.edu/news/news-article/global-maps-magnetic-field-solar-corona</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Global Maps of the Magnetic Field in the Solar Corona&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="2021-11-23T09:05:28-07:00" title="Tuesday, November 23, 2021 - 09:05" class="datetime"&gt;Tue, 11/23/2021 - 09:05&lt;/time&gt;
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        &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 23, 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;An international team led by solar physicists from Peking University, China and National Center for Atmospheric Research (NCAR), USA, has recently measured the global magnetic field of the solar corona for the first time. The team used observations from the Coronal Multi-channel Polarimeter, an instrument operated by NCAR’s High Altitude Observatory. Their results have been published in the Science magazine on August 7, 2020.&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/Model-of-MagneticField.jpg?itok=g5KigS2o" width="926" height="925" alt="Magnetic field of the Sun" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Magnetic field of the Sun calculated from the potential field source surface model (Yang, Tian, Tomczyk et al. 2020, Sci China Tech Sci).&lt;/p&gt;

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


&lt;p&gt;The Sun is a magnetized star, and its magnetic field plays a critical role in shaping the solar atmosphere. The 11-year solar cycle, the spectacular solar eruptions and the million-degree solar corona are all driven or governed by the evolution of the solar magnetic field. Due to the magnetic coupling of different atmospheric layers, information on the magnetic field of the whole atmosphere is required to study the interplay between the solar plasma and magnetic field. However, routine measurements of the solar magnetic field have only been achieved at the photospheric level (solar surface). More than one century has passed since the first measurement of the solar magnetic field, we still do not have a precise knowledge of the magnetic field in the upper solar atmosphere, especially the corona, which impedes our complete understanding of the solar magnetism and its interaction with the solar plasma.&lt;/p&gt;

&lt;p&gt;More than 20 years ago, a technique called coronal seismology or magnetoseismology has been introduced for coronal magnetic field diagnostics. This method makes use of magnetohydrodynamic (MHD) oscillations or waves that are observed in coronal loops or other coronal structures. From the MHD theory, the observed wave parameters can be used to infer the average magnitudes of the magnetic field in the oscillating structures. However, these oscillations/waves are just occasionally observed in small regions of the corona, and thus their potential for magnetic field diagnostics is limited.&lt;/p&gt;


&lt;figure class="align-right 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/CoronalImage-with-MagneticFieldMap.png?itok=pKetmxo9" width="926" height="475" alt="A coronal image and the corresponding magnetic field map" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;A coronal image (left) and the corresponding magnetic field map (right) (Yang, Bethge, Tian, Tomczyk, et al. 2020, Science).&lt;/p&gt;

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


&lt;p&gt;CoMP is a coronagraph with a 20-cm aperture. Using the Fe XIII 1074.7 nm and 1079.8 nm infrared spectral lines, it can observe the solar corona in the range of about 1.05 to 1.35 solar radii from the solar center through imaging spectroscopy and spectropolarimetry. The Doppler image sequence obtained from CoMP observations often reveal the prevalence of propagating periodic disturbances, indicating the ubiquitous presence of transverse MHD waves in the corona. The team has successfully applied the magnetoseismology method to these pervasive waves. They have extended the previously developed wave-tracking technique to the whole field of view, and obtained the global distribution of the wave phase speed. The intensity ratio of the two Fe XIII lines is sensitive to the electron density, thus has been used to derive the global map of coronal electron density. Combing the wave-tracking and density diagnostic results, they have successfully mapped the magnetic field in the global corona.&lt;/p&gt;

&lt;p&gt;This is the first time that a global map of the coronal magnetic field has been obtained through actual coronal observations, thus marking a leap towards solving the problem of coronal magnetic field measurements. In principle, with this technique, global coronal magnetic field maps could now be routinely obtained, filling in the missing part of the measurements of the Sun’s global magnetism. Together with simultaneously measured photospheric magnetograms, these synoptic coronal magnetograms will provide critical information to advance our understanding of the magnetic coupling between different atmospheric layers as well as the physical mechanisms responsible for solar eruptions and solar cycle.&lt;/p&gt;

&lt;p&gt;See write-ups in&amp;nbsp;&lt;a href="https://science.sciencemag.org/content/369/6504/694?fbclid=IwAR2YyJKy6Stn_8gVfGXOgeyR4MFiFUYs7n5Fpt3QKQ7abdorg_5RGHXJ4Ts"&gt;Science&lt;/a&gt;,&amp;nbsp;&lt;a href="https://www.newscientist.com/article/2251150-maps-of-the-suns-corona-could-help-us-predict-dangerous-solar-storms/"&gt;New Scientist&lt;/a&gt;,&amp;nbsp;&lt;a href="https://www.sciencenews.org/article/sun-first-map-solar-corona-magnetic-field"&gt;Science News&lt;/a&gt;&lt;/p&gt;

&lt;div class="resources-main border-0"&gt;
  &lt;a href="https://www2.hao.ucar.edu/sites/default/files/2021-11/Global%20maps%20of%20the%20magnetic%20field%20in%20the%20solar%20corona.pdf" class="i-file-pdf--before" target="_blank"&gt;Global maps of the magnetic field in the solar corona&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/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="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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
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  <pubDate>Tue, 23 Nov 2021 16:05:28 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">101 at https://www2.hao.ucar.edu</guid>
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<item>
  <title> Detecting the Chromospheric Footpoints of the Solar Wind</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/detecting-chromospheric-footpoints-solar-wind</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt; Detecting the Chromospheric Footpoints of the Solar Wind&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="2021-11-16T14:53:48-07:00" title="Tuesday, November 16, 2021 - 14:53" class="datetime"&gt;Tue, 11/16/2021 - 14:53&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: ApJL; Authors: Paul Bryans, Scott McIntosh, David Brooks, Bart De Pontieu&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 16, 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;Coronal Holes present the source of the fast solar wind. However, the fast solar wind is not unimodal—there are discrete, but subtle, compositional, velocity, and density structures that differentiate different coronal holes as well as wind streams that originate within one coronal hole. In this Letter we exploit full-disk observational “mosaics” performed by the Interface Region Imaging Spectrograph (IRIS) spacecraft to demonstrate that significant spectral contrast exists within the chromospheric plasma of coronal holes.&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/Bryans_SDO%20and%20IRIS%20full-disk%20observations.png?itok=dLAeSc-W" width="926" height="1349" alt="SDO and IRIS full-disk observations from 2016 Feb 22" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;SDO and IRIS full-disk observations from 2016 Feb 22. The HMI and AIA Frankenmaps (panels A and B) are constructed of sub-images with the same fields of view and timing of the IRIS rasters that comprise the mosaic. The CHs in the northern hemisphere and at the south pole are most evident in the AIA intensity image (B), but not in Mg II intensity (C). The CHs are evident, however, in the Mg II peak separation map (D). After removing the center-to-limb variation, this is even clearer (F).&lt;/p&gt;

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


&lt;p&gt;The spectral contrast seen delineates topological differences within the globally open structure. In particular, we show that the “peak separation” of the Mg II h line at 2803 A illustrates changes in what appear to be open magnetic features within a coronal hole. These observations point to a chromospheric source for the inhomogeneities found in the fast solar wind. These chromospheric signatures can provide additional constraints on magnetic field extrapolations close to the source, potentially on spatial scales smaller than from traditional coronal hole detection methods based on intensity thresholding in the corona. This is of increased importance with the advent of Parker Solar Probe and Solar Orbiter and the ability to accurately establish the connectivity between their in situ measurements and remote sensing observations of the solar atmosphere.&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;

&lt;/a&gt;
&lt;/div&gt;
      
    &lt;/figure&gt;
  
      &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;
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&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/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;
&lt;/div&gt;
      
    &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;
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&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;
      &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;
  
  
  &lt;/div&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;
&lt;/div&gt;
      
    &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;
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&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/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;
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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/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;
&lt;/div&gt;
      
    &lt;/figure&gt;
  
      &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;
  &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/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;
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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;
&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;
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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/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="2020-11-24T12:00:00Z" class="datetime"&gt;Tue, 11/24/2020 - 12:00&lt;/time&gt;
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  <pubDate>Tue, 16 Nov 2021 21:53:48 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
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