Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/8865
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dc.contributor.authorVemareddy, P-
dc.contributor.authorSelva Bharathi, K-
dc.date.accessioned2026-01-07T06:51:01Z-
dc.date.available2026-01-07T06:51:01Z-
dc.date.issued2025-11-20-
dc.identifier.citationThe Astrophysical Journal, Vol. 994, No. 1, 3en_US
dc.identifier.issn1538-4357-
dc.identifier.urihttp://hdl.handle.net/2248/8865-
dc.descriptionOpen Accessen_US
dc.descriptionOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.-
dc.description.abstractWe investigate the solar origin and heliospheric evolution of an intense geomagnetic storm that occurred on 2023 March 23─24. Despite multiple candidate coronal mass ejections (CMEs) observed between March 19 and 21, a weak CME detected on March 19 at 18:00 UT was identified as the cause, originating from the eruption of a longitudinal-filament channel near the center of the Sun. The channel underwent a smooth transition to the eruption phase without detectable low-coronal signatures. Wide-angle heliospheric imaging revealed asymmetric expansion and acceleration by solar wind drag, achieving an average CME velocity of ≍640 km s−1. The radial evolution of the interplanetary coronal mass ejection (ICME) was analyzed by three spacecraft in close radial alignment. Arrival times and propagation speeds were consistent across spacecraft, with a 21 hr delay between STEREO-A (STA) and WIND attributed to solar rotation and longitudinal separation. The ICME exhibits magnetic cloud (MC) signatures characterized by right-handed helicity, enhanced density at all three spacecraft. The MC underwent expansion (radial-size increases from 0.08 au at SolO to 0.18 au at STA), a decrease in magnetic field strength with distance; Bav∝RH−1.97 (SolO-STA) and Bav∝RH−1.53 (SolO-WIND). The MC axis is inclined with the ecliptic at −69° at SolO, −25° at STA, and −34° at WIND, indicating rotation during heliospheric transit. Importantly, the storm's main phase leads to a peak intensity (SYM-H= −169 nT) occurring at 24/02:40 UT, followed by a second peak (SYM-H = −170 nT) at 24/05:20 UT due to density enhancement toward MC's tail. The study emphasizes the significant geoeffectiveness of weak, stealth CMEs with southward Bz and density enhancements.en_US
dc.language.isoenen_US
dc.publisherAmerican Astronomical Societyen_US
dc.relation.urihttps://doi.org/10.3847/1538-4357/ae0992-
dc.rights© 2025 The Author(s)-
dc.subjectSolar coronal mass ejectionsen_US
dc.subjectSolar-terrestrial interactionsen_US
dc.subjectHeliosphereen_US
dc.subjectSolar stormen_US
dc.titleAn intense geomagnetic storm originated from stealth coronal mass ejection: Remote and in situ observations by near radially aligned spacecraften_US
dc.typeArticleen_US
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