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    <title>spectropolarimetry</title>
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  <title>Erratum: Analysis of Seeing-Induced Polarization Cross-Talk and Modulation Scheme Performance</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/erratum-analysis-seeing-induced-polarization-cross-talk-and-modulation</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Erratum: Analysis of Seeing-Induced Polarization Cross-Talk and Modulation Scheme Performance&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="2024-08-01T09:39:00-06:00" title="Thursday, August 1, 2024 - 09:39" class="datetime"&gt;Thu, 08/01/2024 - 09:39&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 1, 2024&lt;/div&gt;
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        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2024-07/Casini_Graph-polarimetricErrors.png?itok=xoDwv_WK" width="926" height="710" alt="Graph of polarimetric errors" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Corrected Figure 7 of Paper I, showing the polarimetric errors for a stepped waveplate with 150◦ retardance (8-state modulation scheme), with dual-beam analysis, and 10 s integration. For this example, we adopted a non-optimal demodulation scheme consisting of simple additions and subtractions of individual modulated signals.&lt;/p&gt;
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&lt;p&gt;&lt;a href="https://iopscience.iop.org/article/10.1088/0004-637X/757/1/45/meta"&gt;&lt;em&gt;&lt;strong&gt;The Astrophysical Journal&lt;/strong&gt;&lt;/em&gt;&lt;/a&gt;:&amp;nbsp;&lt;em&gt; (Published 2012 September 4; submitting a "corrected" Figure 7 of Paper I)&lt;/em&gt; We analyze the generation of polarization cross-talk in Stokes polarimeters by atmospheric seeing, and its effects on the noise statistics of spectropolarimetric measurements for both single-beam and dual-beam instruments. We investigate the time evolution of seeing-induced correlations between different states of one modulation cycle and compare the response to these correlations of two popular polarization modulation schemes in a dual-beam system. Extension of the formalism to encompass an arbitrary number of modulation cycles enables us to compare our results with earlier work. Even though we discuss examples pertinent to solar physics, the general treatment of the subject and its fundamental results might be useful to a wider community.&lt;/p&gt;&lt;/div&gt;
      
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  <pubDate>Thu, 01 Aug 2024 15:39:00 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">965 at https://www2.hao.ucar.edu</guid>
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<item>
  <title>2nd Successful Spectropolarimetry School</title>
  <link>https://www2.hao.ucar.edu/news/news-article/2nd-successful-spectropolarimetry-school</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;2nd Successful Spectropolarimetry School&lt;/span&gt;
&lt;span class="field field--name-uid field--type-entity-reference field--label-hidden"&gt;&lt;span&gt;whawkins&lt;/span&gt;&lt;/span&gt;
&lt;span class="field field--name-created field--type-created field--label-hidden"&gt;&lt;time datetime="2022-09-07T09:36:21-06:00" title="Wednesday, September 7, 2022 - 09:36" class="datetime"&gt;Wed, 09/07/2022 - 09:36&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;2022 Spectropolarimetry School&lt;/p&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 7, 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;The High Altitude Observatory and the National Solar Observatory organized their second successful Spectropolarimetry School in Boulder, Colorado. This two-week school held at the end of August presented an overview of the field of solar spectropolarimetry and the diagnostic techniques used to analyze and interpret spectropolarimetric observations of the Sun.&lt;/p&gt;

&lt;p&gt;Solar magnetism is at the root of all solar activity and is the driving force of Space Weather. The characteristics of the magnetic field are encoded in the polarization of the light emitted by the Sun, and sensitive analysis techniques are necessary to reveal them. This school explored the observations, the theory and the tools that help us determine the state and evolution of the Sun's magnetic field through its polarized spectrum. The curriculum covered theoretical topics such as polarized radiative transfer, polarimetric instrumentation, scattering polarization and the Hanle effect, as well as dozens of hours of hands-on tutorials with different spectral line inversion codes. The school brought together 19 domestic and 7 international participants as well as multiple leading experts from around the world.&lt;/p&gt;


&lt;figure class="media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2022-09/HelioSchoolGroupPhoto.jpg?itok=iesSSX9w" width="926" height="546" alt="Smiling group of Spectropolarimetry school students and lecturers taken on the outdoor patio at Center Green 1 building." class="image-style-extra-large img-fluid"&gt;



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          &lt;p&gt;Group portrait of the 2022 Spectropolarimetry school students and lecturers taken on the outdoor patio at Center Green 1 building.&lt;/p&gt;

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      &lt;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Dec 11, 2025&lt;/div&gt;
  
  
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&lt;/a&gt;
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      &lt;div class="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;div class="pb-1 text-gray-dark text-uppercase date--sm"&gt;Aug 13, 2025&lt;/div&gt;
  
  
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              &lt;div class="field__item"&gt;&lt;time datetime="2022-08-31T12:00:00Z" class="datetime"&gt;Wed, 08/31/2022 - 12:00&lt;/time&gt;
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/66" hreflang="en"&gt;Rebecca Centeno&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/41" hreflang="en"&gt;spectropolarimetry&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Wed, 07 Sep 2022 15:36:21 +0000</pubDate>
    <dc:creator>whawkins</dc:creator>
    <guid isPermaLink="false">696 at https://www2.hao.ucar.edu</guid>
    </item>
<item>
  <title>On the (Mis)interpretation of the Scattering Polarization Signatures In the Ca II 8542 A line Through Spectral Line Inversions</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/misinterpretation-scattering-polarization-signatures-ca-ii-8542-line</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;On the (Mis)interpretation of the Scattering Polarization Signatures In the Ca II 8542 A line Through Spectral Line Inversions&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="2022-07-11T14:45:28-06:00" title="Monday, July 11, 2022 - 14:45" class="datetime"&gt;Mon, 07/11/2022 - 14:45&lt;/time&gt;
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      &lt;p class="field field--name-field-subtitle field--type-string field--label-above mb-4"&gt;Publication Name: The Astrophysical Journal; Author's names: Centeno, R., de la Cruz Rodriguez, J., del Pino Aleman, T.&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;Jul 11, 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;Scattering polarization tends to dominate the linear polarization signals of the Ca II 8542 A line in weakly magnetized areas (B ~ 100 G), especially when the observing geometry is close to the limb. In this paper we evaluate the degree of applicability of existing non-LTE spectral line inversion codes (which assume that the spectral line polarization is due to the Zeeman effect only) at inferring the magnetic field vector and, particularly, its transverse component. To this end, we use the inversion code STiC to extract the strength and orientation of the magnetic field from synthetic spectropolarimetric data generated with the Hanle-RT code. The latter accounts for the generation of polarization through scattering processes as well as the joint actions of the Hanle and the Zeeman effects. We find that, when the transverse component of the field is stronger than ~80 G, the inversion code is able to retrieve accurate estimates of the transverse field strength as well as its azimuth in the plane of the sky. Below this threshold, the scattering polarization signatures become the major contributors to the linear polarization signals and often mislead the inversion code into severely over- or under-estimating the field strength. Since the line-of-sight component of the field is derived from the circular polarization signal, which is not affected by atomic alignment, the corresponding inferences are always good.&lt;/p&gt;


&lt;figure class="align-center 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/2022-07/Centeno-inversion-results.png?itok=yGxsZGQQ" width="926" height="668" alt="Inversion results for observing geometries away from the disk center" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Inversion results for observing geometries away from the disk center. The panels show the relative (percent) differences between the magnetic field values retrieved by the STiC inversions and those in the model atmospheres used for the Hanle-RT syntheses. Left and right correspond, respectively, to the Zeeman-only and the full calculation with atomic polarization cases. The top two rows show the results for the strength and the azimuth of the transverse component of the magnetic field, while the bottom panels present the results for the LOS magnetic field.&lt;/p&gt;

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

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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/66" hreflang="en"&gt;Rebecca Centeno&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/14" hreflang="en"&gt;solar magnetism&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/41" hreflang="en"&gt;spectropolarimetry&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Mon, 11 Jul 2022 20:45:28 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">597 at https://www2.hao.ucar.edu</guid>
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  <title>Efficient and Automated Inversions of Magnetically-Sensitive Forbidden Coronal Lines: CLEDB - The Coronal Line Emission DataBase Magnetic Field Inversion Algorithm</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/efficient-and-automated-inversions-magnetically-sensitive-forbidden</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Efficient and Automated Inversions of Magnetically-Sensitive Forbidden Coronal Lines: CLEDB - The Coronal Line Emission DataBase Magnetic Field Inversion Algorithm&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="2022-07-11T14:24:06-06:00" title="Monday, July 11, 2022 - 14:24" class="datetime"&gt;Mon, 07/11/2022 - 14:24&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;Jul 11, 2022&lt;/div&gt;
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              &lt;div class="field__item"&gt;  &lt;div class="paragraph paragraph--type--rich-text paragraph--view-mode--default"&gt;
          
            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;Alin Paraschiv and Philip Judge present CLEDB, a single point inversion algorithm for determining magnetic parameters using spectro-polarimetric measurements of emission lines formed in the solar corona. We select lines of interest and construct databases for combinations of plasma thermal and magnetic configurations. The method is intended to be applied to two or more lines observed simultaneously. The solutions initially yield magnetic orientation, thermal properties, and the spatial position of the emitting plasma in three dimensions. Multiple possible solutions for each observation are returned, including irreducible degeneracies. The magnetic field strength is separately derived from the simple ratio of observed to database polarization data, after the thermal properties and scattering geometry solutions have been determined.&lt;/p&gt;


&lt;figure class="media media--type-image media--view-mode-default figure mb-1 mb-md-4"&gt;
  
        &lt;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2022-07/Paraschiv_magneticInversionAlgorithmFlowchart.png?itok=S7VRB_d1" width="926" height="414" alt="CLEDB 2-line magnetic inversion algorithm flowchart. An important aspect is the delivery of multiple possible solutions for each observation at the last step. Note that the x-coordinate of the point in space, as well as nearest electron density, are returned along with B. The figure uses the notation Vobs and Vdb for observed and computed values of the amplitudes of the Stokes parameters corresponding to O3 and S3 (B = 1) in the text." class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;CLEDB 2-line magnetic inversion algorithm flowchart. An important aspect is the delivery of multiple possible solutions for each observation at the last step. Note that the x-coordinate of the point in space, as well as nearest electron density, are returned along with B. The figure uses the notation Vobs and Vdb for observed and computed values of the amplitudes of the Stokes parameters corresponding to O3 and S3 (B = 1) in the text.&lt;/p&gt;

          &lt;/figcaption&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/10" hreflang="en"&gt;Phil Judge&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/3" hreflang="en"&gt;corona&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/14" hreflang="en"&gt;solar magnetism&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/41" hreflang="en"&gt;spectropolarimetry&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Mon, 11 Jul 2022 20:24:06 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">594 at https://www2.hao.ucar.edu</guid>
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  <title>A Spectroscopic Survey of Infrared 1–4 μm Spectra in Regions of Prominent Solar Coronal Emission Lines of Fe XIII, Si X, and Si IX</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/spectroscopic-survey-infrared-1-4-mm-spectra-regions-prominent-solar</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;A Spectroscopic Survey of Infrared 1–4 μm Spectra in Regions of Prominent Solar Coronal Emission Lines of Fe XIII, Si X, and Si IX&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="2022-07-11T12:57:40-06:00" title="Monday, July 11, 2022 - 12:57" class="datetime"&gt;Mon, 07/11/2022 - 12:57&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: The Astrophysical Journal; Authors: Aatiya Ali, Alin Razvan Paraschiv, Kevin Reardon, and 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;Jul 11, 2022&lt;/div&gt;
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              &lt;div class="field__item"&gt;  &lt;div class="paragraph paragraph--type--rich-text paragraph--view-mode--default"&gt;
          
            &lt;div class="clearfix text-formatted field field--name-field-body field--type-text-long field--label-hidden field__item"&gt;&lt;p&gt;The infrared solar spectrum contains a wealth of physical data about the Sun and is being explored using modern detectors and technology with new ground-based solar telescopes. One such instrument will be the ground-based Cryogenic Near-IR Spectro-Polarimeter of the Daniel K. Inouye Solar Telescope (DKIST), which will be capable of sensitive imaging of the faint infrared solar coronal spectra with full Stokes polarization states. Highly ionized emission lines have been observed in galaxies and the solar corona. Quantifying the accuracy of spectral inversion procedures requires a precise spectroscopic calibration of observations. A careful interpretation of the spectra around prominent magnetic dipole lines is essential for deriving physical parameters and particularly for quantifying the off-limb solar coronal observations from DKIST. In this work, we aim to provide an analysis of the spectral regions around the infrared coronal emission lines of Fe xiii 1074.68 nm, Fe xiii 1079.79 nm, Si x 1430.10 nm, and Si ix 3934.34 nm, aligning with the goal of identifying solar photospheric and telluric lines that will help facilitate production of reliable inversions and data products from four sets of solar coronal observations.&lt;/p&gt;


&lt;figure class="align-center 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/2022-07/Paraschiv_FE_XIII.jpg?itok=iVT2uPak" width="926" height="619" alt="Fe XIII 1074.68 nm emission over atmospheric absorption (normalized) in the He I Cryo-NIRSP wavelength range with all labeled candidate lines." class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Fe XIII 1074.68 nm emission over atmospheric absorption (normalized) in the He I Cryo-NIRSP wavelength range with all labeled candidate lines. The green curve represents the atmospheric spectra that are convolved with a Gaussian function correspondent to the Cryo-NIRSP 0"5 slit spectral resolution of 0.027 nm.&lt;/p&gt;

          &lt;/figcaption&gt;
  &lt;/figure&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/10" hreflang="en"&gt;Phil Judge&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/3" hreflang="en"&gt;corona&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/42" hreflang="en"&gt;instrumentation&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/41" hreflang="en"&gt;spectropolarimetry&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Mon, 11 Jul 2022 18:57:40 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
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<item>
  <title>Multiwavelength High-resolution Observations of Chromospheric Swirls in the Quiet Sun</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/multiwavelength-high-resolution-observations-chromospheric-swirls-quiet</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Multiwavelength High-resolution Observations of Chromospheric Swirls in the Quiet Sun&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="2021-11-18T12:07:10-07:00" title="Thursday, November 18, 2021 - 12:07" class="datetime"&gt;Thu, 11/18/2021 - 12:07&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: ApJ 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 report observations of small-scale swirls seen in the solar chromosphere. They are typically 2 Mm in diameter and last around 10 minutes. Using spectropolarimetric observations obtained by the CRisp Imaging Spectro- Polarimeter at the Swedish 1 m Solar Telescope, we identify and study a set of swirls in chromospheric Ca II 8542 Å and Hα lines as well as in the photospheric Fe I line.&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_swirls.png?itok=T-L_RX_Z" width="926" height="478" alt="Selected swirling events" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Snapshots in Hα 6563 Å, Ca II 8542.11 Å, and Stokes-V of Fe 6302 Å, and Doppler difference images constructed in Ca II 8542 Å showing selected swirling events.&lt;/p&gt;

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


&lt;p&gt;We have three main areas of focus. First, we compare the appearance, morphology, dynamics, and associated plasma parameters between the Ca II and Hα channels. Rotation and expansion of the chromospheric swirl pattern are explored using polar plots. Second, we explore the connection to underlying photospheric magnetic concentration (MC) dynamics. MCs are tracked using the SWAMIS tracking code. The swirl center and MC remain cospatial and share similar periods of rotation. Third, we elucidate the role swirls play in modifying chromospheric acoustic oscillations and found a temporary reduction in wave period during swirls. We use cross-correlation wavelets to examine the change in period and phase relations between different wavelengths. The physical picture that emerges is that a swirl is a flux tube that extends above an MC in a downdraft region in an intergranular lane. The rotational motion of the MC matches the chromospheric signatures.&lt;/p&gt;
&lt;/div&gt;
      
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              &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/10" hreflang="en"&gt;Phil Judge&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/4" hreflang="en"&gt;chromosphere&lt;/a&gt;,       &lt;a href="https://www2.hao.ucar.edu/taxonomy/term/41" hreflang="en"&gt;spectropolarimetry&lt;/a&gt;        &lt;/div&gt;
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  <pubDate>Thu, 18 Nov 2021 19:07:10 +0000</pubDate>
    <dc:creator>kolinski</dc:creator>
    <guid isPermaLink="false">80 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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  <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>Design of a Highly Efficient Polychromatic Full-Stokes Polarization Modulator for the CRISP Imaging Spectrometer</title>
  <link>https://www2.hao.ucar.edu/news/publication-highlight/design-highly-efficient-polychromatic-full-stokes-polarization-modulator</link>
  <description>&lt;span class="field field--name-title field--type-string field--label-hidden"&gt;Design of a Highly Efficient Polychromatic Full-Stokes Polarization Modulator for the CRISP Imaging Spectrometer&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="2021-11-16T14:14:23-07:00" title="Tuesday, November 16, 2021 - 14:14" class="datetime"&gt;Tue, 11/16/2021 - 14:14&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: ApJ; First HAO Author: Alfred de Wijn; Authors as listed in article: A.G. de Wijn, J. de la Cruz Rodríguez, G.B. Scharmer, G. Sliepen, and P. Sütterlin&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;img loading="lazy" src="https://www2.hao.ucar.edu/sites/default/files/styles/extra_large/public/2021-11/DeWijn_spectro-polarimetric%20data_fig_spot_6302.png?itok=oTsdBls4" width="926" height="405" alt="Example spectro-polarimetric data of Active Region 12471 in the Fe I lines at 630.2 nm" class="image-style-extra-large img-fluid"&gt;



      &lt;figcaption class="figure-caption pb-1"&gt;
          &lt;p&gt;Example spectro-polarimetric data of Active Region 12471 in the Fe I lines at 630.2 nm. The observation was recorded on 2019-05-10 around 09:10 UT. Top row: images of the Stokes parameter in the blue wing of the 630.25 nm line at −90 mÅ from line center. Spectra at the black, red, and blue crosses are shown in the bottom row. The locations of the spectral sampling are indicated by crosses.&lt;/p&gt;

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


&lt;p&gt;In 2014 HAO built a polarimetric modulator for the CRISP instrument on the Swedish 1-m Solar Telescope in La Palma, using the principles of polychromatic modulation previously developed by HAO scientists. This paper discusses the processes by which the modulator was designed, built, and tested. The modulator was installed and had been in use since 2015. It is working at close to optimal efficiency and has produced considerable scientific output.&lt;/p&gt;

&lt;p&gt;Link to paper:&amp;nbsp;&lt;a href="https://iopscience.iop.org/article/10.3847/1538-3881/abd2b1"&gt;Design and Performance Analysis of a Highly Efficient Polychromatic Full Stokes Polarization Modulator for the CRISP Imaging Spectrometer&lt;/a&gt;&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;
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    &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="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="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;
&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;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;
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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;
  &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/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;
      &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/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;
&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="2021-02-02T12:00:00Z" class="datetime"&gt;Tue, 02/02/2021 - 12:00&lt;/time&gt;
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  <pubDate>Tue, 16 Nov 2021 21:14:23 +0000</pubDate>
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