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    <title>CME</title>
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  <title>Magnetic field and plasma diagnostics for solar coronal mass ejections: A case study using the forward modeling approach</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/magnetic-field-and-plasma-diagnostics-solar-coronal-mass-ejections-case</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Magnetic field and plasma diagnostics for solar coronal mass ejections: A case study using the forward modeling approach&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="2023-03-03T15:05:34-07:00" title="Friday, March 3, 2023 - 15:05" class="datetime"&gt;Fri, 03/03/2023 - 15:05&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;Mar 3, 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/2023-03/Liu_Fe-xiii-10747-line%2BCME-eruptions.jpg?itok=LUMaZKJO" width="926" height="685" alt="Liu Fe xiii 10747 line and CME eruption" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Synthesized results of the Fe xiii 10747 line, along with several POS cross section quantities in the model during CME eruption (a)-(e): Intensity (Stokes I), linear polarization degree(L/I), line width, Doppler velocity, and azimuth derived from synthesized signals. (f)-(h): Magnetic field, temperature, and density distributions in the POS. The arc-shaped contour in each panel represents ∇ · v = −0.05. Two leading fronts (LF) can be distinguished in panel (a). Each white arrow in panel (g) represents the POS projection of the deduced shock normals. The solar disk is indicated by the yellow curve in each panel. The region below 1.05R⊙ is masked.&lt;/p&gt;

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&lt;p&gt;&lt;strong&gt;&lt;em&gt;&lt;a href="https://link.springer.com/article/10.1007/s11207-023-02207-5"&gt;Solar Physics&lt;/a&gt;&lt;/em&gt;&lt;/strong&gt;:&amp;nbsp; The proposed COronal Solar Magnetism Observatory (COSMO) Large Coronagraph (LC) will provide unique observations to study coronal mass ejections (CMEs) with its ability to diagnose the magnetic field and plasma properties in the solar corona. Here we take a realistic magnetohydrodynamic CME model, and synthesize the signals of several coronal emission lines (CELs) to perform forward modeling of COSMO LC observation of a CME. We use the Stokes parameters of the Fe xiii 10747 Angstrom line to diagnose the magnetic field and plasma properties of the CME flux rope. The results show that COSMO LC can provide magnetic field measurements of CME progenitors with a high spatial resolution (2′′ pixels). By using a worse resolution (6′′ pixels), the COSMO LC observation may also be used to qualitatively study the evolution of magnetic field during the CME eruption. We then use the synthetic signals of several other CELs to diagnose the physical conditions in the CME leading front, including the shock. The COSMO LC observations of the Fe xiii 10798/10747 Angstrom and Ar xiii 8300/10143 Angstrom line pair can provide density diagnostics of the front. By observing several CELs with different formation temperatures, the COSMO LC can be used to diagnose the temperature and ionization states in the front. We suggest that the Fe xiii 10747 Angstrom line should be given the highest priority when observing CMEs, while observations of the Fe xiii 10798 Angstrom, Fe xiv 5303 Angstrom, Fe xv 7062 Angstrom, and Ar xiii 10143 Angstrom lines can also provide valuable information on CMEs.&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;
  
  
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    &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="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;
  
  
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    &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;
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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;

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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/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;
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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="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="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;
  
  
  &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;
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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;
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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;
  
  
  &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;
    &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;
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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="2023-10-03T12:00:00Z" class="datetime"&gt;Tue, 10/03/2023 - 12:00&lt;/time&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/15" hreflang="en"&gt;Sarah Gibson&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/55" hreflang="en"&gt;CME&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/69" hreflang="en"&gt;COSMO&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/13" hreflang="en"&gt;modeling&lt;/a&gt;        &lt;/div&gt;
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</description>
  <pubDate>Fri, 03 Mar 2023 22:05:34 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">800 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>Predicting the Geoeffectiveness of CMEs Using Machine Learning</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/predicting-geoeffectiveness-cmes-using-machine-learning</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Predicting the Geoeffectiveness of CMEs Using Machine Learning&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;whawkins&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2022-08-23T09:59:37-06:00" title="Tuesday, August 23, 2022 - 09:59" class="datetime"&gt;Tue, 08/23/2022 - 09:59&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;Aug 23, 2022&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2022-08/Paraschiv_UMAP.jpg?itok=N4mbdx5L" width="926" height="412" alt="A graph showing colored dots representing: True Negative; False Positive; True Positive, False Negative" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;UMAP of the predictions of the ensemble model, applied on the test set (20% of the data), colored by their correctness. Labels: TN - True Negative; FP - False Positive; TP - True Positive; FN - False Negative.&lt;/p&gt;

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


&lt;p&gt;Coronal mass ejections are the most important space weather phenomena, being associated with large geomagnetic storms, and having the potential to cause disturbances to telecommunications, satellite network disruptions, and power grid damage and failures. Thus, considering these storms' potential effects on human activities, accurate forecasts of the geoeffectiveness of CMEs are paramount. This work focuses on experimenting with different machine-learning methods trained on data sets of close-to-Sun CMEs, to estimate whether such a newly erupting ejection has the potential to induce geomagnetic activity. We developed classification models using a variety of machine learning approaches. At this time, we limited our forecast to exclusively use solar onset parameters, to ensure extended warning times. We discuss the main challenges of this task and show that adequate predictions can be achieved with these models.&lt;/p&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="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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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/99" hreflang="en"&gt;Alin Razvan Paraschiv&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/55" hreflang="en"&gt;CME&lt;/a&gt;        &lt;/div&gt;
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</description>
  <pubDate>Tue, 23 Aug 2022 15:59:37 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">677 at https://www2.hao.ucar.edu</guid>
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  <title>Spectropolarimetric Insight into Plasma-Sheet Dynamics of a Solar Flare</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/spectropolarimetric-insight-plasma-sheet-dynamics-solar-flare</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Spectropolarimetric Insight into Plasma-Sheet Dynamics of a Solar Flare&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="2021-11-18T12:02:39-07:00" title="Thursday, November 18, 2021 - 12:02" class="datetime"&gt;Thu, 11/18/2021 - 12:02&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: ApJL; First HAO Author's Name: Philip Judge&lt;/p&gt;

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        &lt;div class="fw-bold fs-6"&gt;Author:&lt;/div&gt;
        &lt;div class="author_created__name fs-6"&gt;kolinski&lt;/div&gt;
                  &lt;div class="author_created__date text-gray-dark fs-6"&gt;Nov 18, 2021&lt;/div&gt;
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            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;We examine spectropolarimetric data from the CoMP instrument, acquired during the evolution of the September 10th 2017 X8.2 solar flare on the western solar limb. CoMP captured linearly polarized light from two emission lines of Fe XIII at 1074.7 and 1079.8 nm, from 1.03 to 1.5 solar radii. We focus here on the hot plasma-sheet lying above the bright flare loops and beneath the ejected CME.&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/Judge_cross_section.png?itok=lk4xYlzG" width="926" height="1273" alt="Intensity and polarization data surrounding the current sheet formed on Sept 10 2017" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Intensity and polarization data surrounding the current sheet formed on Sept 10 2017.&lt;/p&gt;

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


&lt;p&gt;The polarization has a striking and coherent spatial structure, with unexpectedly small polarization aligned with the plasma-sheet. By elimination, we find that small-scale magnetic field structure is needed to cause such significant depolarization, and suggest that plasmoid formation during reconnection (associated with the tearing mode instability) creates magnetic structure on scales below instrument resolution of 6 Mm. We conclude that polarization measurements with new coronagraphs, such as the upcoming DKIST, will further enhance our understanding of magnetic reconnection and development of turbulence in the solar corona.&lt;/p&gt;
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&lt;/a&gt;
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  <pubDate>Thu, 18 Nov 2021 19:02:39 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">79 at https://www2.hao.ucar.edu</guid>
    </item>
<item>
  <title>Convolutional Neural Networks for Predicting the strength of the Near-Earth Magnetic Field Caused by Interplanetary Coronal Mass Ejections</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/convolutional-neural-networks-predicting-strength-near-earth-magnetic</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Convolutional Neural Networks for Predicting the strength of the Near-Earth Magnetic Field Caused by Interplanetary Coronal Mass Ejections&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;kolinski&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2021-11-17T09:26:43-07:00" title="Wednesday, November 17, 2021 - 09:26" class="datetime"&gt;Wed, 11/17/2021 - 09:26&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: Frontiers in Astronomy; Authors names as they are listed in article: Anna Malanushenko, Natasha Flyer, Sarah Gibson&lt;/p&gt;

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


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



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

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


&lt;p&gt;The GLOW model is used as a first simple test of a self-similarly expanding magnetic flux rope which nevertheless allows consideration of the impact of varying CME location, orientation, size, and morphology. The CNN problem is set up in two experiments: 1) given input data near the Sun, three 2D images in the meridional plane of the components of the magnetic field, predict the maximal southward amplitude of the measured magnetic field at the Earth; 2) given line-of-sight integrated images of the Stokes parameters, corresponding to the physical configurations of the over 30K flux ropes from Part 1, predict the maximal southward amplitude of the measured magnetic field at the Earth.&lt;/p&gt;
&lt;/div&gt;
      
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&lt;/a&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/54" hreflang="en"&gt;Anna Malanushenko&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/55" hreflang="en"&gt;CME&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/53" hreflang="en"&gt;GLOW&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/2" hreflang="en"&gt;magnetosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/13" hreflang="en"&gt;modeling&lt;/a&gt;        &lt;/div&gt;
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