X-ray and radio manifestations of a solar eruptive event

Citation
N. Gopalswamy et al., X-ray and radio manifestations of a solar eruptive event, ASTRON ASTR, 347(2), 1999, pp. 684-695
Citations number
25
Categorie Soggetti
Space Sciences
Journal title
ASTRONOMY AND ASTROPHYSICS
ISSN journal
00046361 → ACNP
Volume
347
Issue
2
Year of publication
1999
Pages
684 - 695
Database
ISI
SICI code
0004-6361(199907)347:2<684:XARMOA>2.0.ZU;2-C
Abstract
e report on a study of the changes in the vicinity of a disappearing solar filament (DSF) that occurred on 1993 April 30. The DSF was associated with a long duration X-ray event (LDE) observed by the GOES and Yohkoh spacecraf t. A detailed analysis of the X-ray images obtained by the Yohkoh Soft Xray Telescope revealed that X-ray manifestations of the eruption were wide-spr ead: (i) X-ray enhancement over a coronal volume several times larger than that of the eruption region, probably the X-ray counterpart of a coronal ma ss ejection (CME), (ii) Xray ejecta accelerating to 670 km s(-1) into the c orona, and (iii) quasi-stationary X-ray loops as in long decay events (LDEs ) were observed. One of the important findings of this study is the large-s cale X-ray enhancement which we identify with the frontal structure of a CM E, apart from the well-known X-ray ejecta and post-eruption arcade formatio n. There is evidence for triggering of a sympathetic flare in an adjoining active region due to the X-ray ejecta from the eruption region. Stationary metric radio continuum observed by the Nancay Radioheliograph was found to be associated with the brightest X-ray loops that formed following the fila ment eruption. The unpolarized continuum radio emission was found to be bre msstrahlung radiation from the hot plasma observed in X-rays. The event was also associated with a low frequency metric type II radio burst due to a c oronal shock wave from the eruption region. The onset time of the type II e mission precludes the possibility of a CME-driven shock causing it. Althoug h we do not have positional information for the type II burst, we found tha t the X-ray ejecta was fast enough to drive the coronal shock. We confirmed this by comparing the speed of the X-ray ejecta with the shock speed obtai ned from the radio data which agreed within 10%.