Y. Hanaoka et al., SIMULTANEOUS OBSERVATIONS OF A PROMINENCE ERUPTION FOLLOWED BY A CORONAL ARCADE FORMATION IN RADIO, SOFT X-RAYS, AND H-ALPHA, Publications of the Astronomical Society of Japan, 46(2), 1994, pp. 205
A prominence eruption followed by a coronal brightening was simultaneo
usly observed in radio (17 GHz), soft X-rays, and Halpha on 1992 July
30-31. The observations were performed by newly developed high-perform
ance instruments: the Nobeyama Radioheliograph, the SXT on the Yohkoh
satellite, the Flare Monitoring Telescope of the Hida Observatory, and
some other Halpha telescopes. This event gives us a much more detaile
d picture of this type of phenomena than previously observed. The erup
ting prominence, which occurred in a quiet region and was observed in
Halpha and radio, ascended with a velocity of about 100 km s-1. The ge
neral structure of the erupting prominence seen at 17 GHz is very simi
lar to that at Halpha. While the prominence expanded rapidly, the tota
l radio flux of the erupting prominence did not change very much. Sinc
e a prominence consists of fine threads, this fact means that each thr
ead did not expand while the prominence expanded. Consequently, the su
rface filling factor of the prominence must have decreased during the
eruption. The high-resolution pictures of a clear coronal arcade struc
ture were taken in soft X-rays and radio after the prominence eruption
; the physical parameters of the arcade were derived from these pictur
es. The mean temperature was 3.5 x 10(6) K in the early phase, and dec
reased to 2.6 x 10(6) K within seven hours. The total emission measure
reached a maximum value of 1.6 x 10(48) CM-3 after three hours from t
he beginning of the arcade brightening, when the electron density at t
he ridge of the arcade is estimated as 2.4 x 10(9) CM-3. The temporal
and spatial relationship between the erupting prominence and the coron
al arcade is shown. It gives an observational restriction to the magne
tic field configuration of the models of such events.