4.7 Article

New evidence for the role of emerging flux in a solar filament's slow rise preceding its CME-producing fast eruption

期刊

ASTROPHYSICAL JOURNAL
卷 669, 期 2, 页码 1359-1371

出版社

IOP PUBLISHING LTD
DOI: 10.1086/520829

关键词

sun : coronal mass ejections (CMEs); sun : filaments; sun : flares; sun : UV radiation; sun : x-rays; gamma rays

资金

  1. STFC [PP/E001173/1] Funding Source: UKRI
  2. Science and Technology Facilities Council [PP/E001173/1] Funding Source: researchfish

向作者/读者索取更多资源

We observe the eruption of a large-scale ( approximate to 300,000 km) quiet-region solar filament leading to an Earth-directed halo'' coronal mass ejection (CME), using data from EIT, CDS, MDI, and LASCO on SOHO and from SXT on Yohkoh. Initially the filament shows a slow ( similar to 1 km s(-1) projected against the solar disk) and approximately constant velocity rise for about 6 hr, before erupting rapidly, reaching a velocity of similar to 8 km s(-1) over the next approximate to 25 minutes. CDS Doppler data show Earth-directed filament velocities ranging from < 20 km s(-1) ( the noise limit) during the slow-rise phase, to similar to 100 km s(-1) early in the eruption. Beginning within 10 hr prior to the start of the slow rise, localized new magnetic flux emerged near one end of the filament. Near the start of and during the slow-rise phase, soft X-ray (SXR) microflaring occurred repeatedly at the flux-emergence site, and the magnetic arcade over the filament progressively brightened in a fan of illumination in SXRs. These observations are consistent with tether-weakening'' reconnection occurring between the newly emerging flux and the overlying arcade field containing the filament, and apparently this reconnection is the cause of the filament's slow rise. We cannot, however, discern whether the transition from slow rise to fast eruption was caused by a final episode of tether-weakening reconnection, or by one or some combination of other possible mechanisms allowed by the observations. Intensity dimmings'' and brightenings'' occurring both near to and relatively far from the location of the filament are possible signatures of the expansion (opening'') of the erupting field and its reconnection with overarching field during the eruption.

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