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  <controlfield tag="001">7956</controlfield>
  <controlfield tag="005">20260213104926.0</controlfield>
  <datafield tag="037" ind1=" " ind2=" ">
    <subfield code="a">SEMIN-2026-0017</subfield>
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  <datafield tag="100" ind1=" " ind2=" ">
    <subfield code="a">Binal, Patel</subfield>
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  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Exploring source regions of coronal mass ejections through multi-wavelength observations</subfield>
  </datafield>
  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2025</subfield>
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  <datafield tag="269" ind1=" " ind2=" ">
    <subfield code="c">2025-11-05</subfield>
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  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">Coronal Mass Ejections (CMEs) are large-scale eruptive phenomena originating from the Sun, primarily observed as outward propagating structures in the white-light coronagraph images. The CME occurs in closed magnetic field regions on the Sun such as active regions, filament regions, transequatorial interconnection regions, and complexes involving a combination of these. Exploring the pre-eruption state of the solar sources of CMEs is a key aspect in unveiling the mechanism involved in CME initiation. In this talk, I will present the investigation of three representative class of CME structures at the source regions: (i) magnetic-arc-blowout CMEs driven by homologous compact blowout jets, (ii) a halo CME produced in association with a large two-ribbon flare, (iii) a hot flux rope eruption in association with blowout expansion of overlying coronal loops. By conducting a thorough multi-wavelength imaging and coronal magnetic field modeling, we shed light on the activation and formation of CME structure within the corona. Our studies provide evidence toward the role of large-scale magnetic fields - both closed and open - in channelizing or constraining the CME’s morphological and dynamics evolution at the near-Sun region. Our studies suggest that the configuration of overlying/surrounding coronal loops in the pre-CME phase and their subsequent interactions with the expanding flux rope plays a decisive role in the formation of CME’s large-scale structure.</subfield>
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  <datafield tag="594" ind1=" " ind2=" ">
    <subfield code="a">STCE</subfield>
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  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="t">Royal Observatory of Belgium</subfield>
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  <datafield tag="856" ind1="0" ind2=" ">
    <subfield code="f">binal.patel@ksb-orb.be</subfield>
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  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="a">SEMIN</subfield>
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