SIMULTANEOUS EXTREME-ULTRAVIOLET EXPLORER AND OPTICAL OBSERVATIONS OFAD LEONIS - EVIDENCE FOR LARGE CORONAL LOOPS AND THE NEUPERT EFFECT IN STELLAR FLARES
Sl. Hawley et al., SIMULTANEOUS EXTREME-ULTRAVIOLET EXPLORER AND OPTICAL OBSERVATIONS OFAD LEONIS - EVIDENCE FOR LARGE CORONAL LOOPS AND THE NEUPERT EFFECT IN STELLAR FLARES, The Astrophysical journal, 453(1), 1995, pp. 464-479
We report on the first simultaneous Extreme-Ultraviolet Explorer (EUVE
) and optical observations of flares on the dMe flare star AD Leonis.
The data show the following features: 1. Two flares (one large and one
of moderate size) of several hours duration were observed in the EUV
wavelength range; 2. Flare emission observed in the optical precedes t
he emission seen with EUVE; 3. Several diminutions (DIMs) in the optic
al continuum were observed during the period of optical flare activity
. To interpret these data, we develop a technique for deriving the cor
onal loop length from the observed rise and decay behavior of the EUV
flare. The technique is generally applicable to existing and future co
ronal observations of stellar flares. We also determine the pressure,
column depth, emission measure, loop cross-sectional area, and peak th
ermal energy during the two EUV flares, and the temperature, area cove
rage, and energy of the optical continuum emission. When the optical a
nd coronal data are combined, we find convincing evidence of a stellar
''Neupert effect'' which is a strong signature of chromospheric evapo
ration models. We then argue that the known spatial correlation of whi
te-light emission with hard X-ray emission in solar flares, and the id
entification of the hard X-ray emission with nonthermal bremsstrahlung
produced by accelerated electrons, provides evidence that flare heati
ng on dMe stars is produced by the same electron precipitation mechani
sm that is inferred to occur on the Sun. We provide a thorough picture
of the physical processes that are operative during the largest EUV f
lare, compare and contrast this picture with the canonical solar flare
model, and conclude that the coronal loop length may be the most impo
rtant factor in determining the flare rise time and energetics.