Bibcode
DOI
Lites, B. W.; Low, B. C.; Martinez Pillet, V.; Seagraves, P.; Skumanich, A.; Frank, Z. A.; Shine, R. A.; Tsuneta, S.
Referencia bibliográfica
Astrophysical Journal v.446, p.877
Fecha de publicación:
6
1995
Número de citas
230
Número de citas referidas
208
Descripción
We present a comprehensive interpretation of the evolution of a small
magnetic region observed during its entire disk passage. The vector
magnetic field measurements from the Advanced Stokes Polarimeter, along
with Hα and magnetogram measurements from the Lockheed SOUP
instrument operating at the Swedish Solar Observatory on La Palma, and
soft X-ray images from the Yohkoh satellite support the hypothesis that
we have observed the passage of a nearly closed magnetic system through
the photosphere into the corona. The observations suggest that as the
magnetic flux begins to emerge into the photosphere it shows a rather
simple geometry, but it subsequently develops a small δ-sunspot
configuration with a highly sheared vector field along the polarity
inversion line running through it. At that stage, the vector field is
consistent with a concave upward magnetic topology, indicative of strong
electric currents above the photosphere. An Hα prominence is found
above this inversion line when the δ-sunspot is fully formed.
These observed features and the sequence of events are interpreted in
terms of a nearly closed magnetic system that rises through the
photosphere into the corona as a result of magnetic buoyancy. The
magnetic system persists in the corona well after the dark
δ-sunspot has disappeared in the photosphere We suggest that this
coronal structure is in quasi-static equilibrium with its buoyancy
partially countered by the weight of the plasma trapped at the bottom of
closed magnetic loops. The plausibility of such a scenario is
demonstrated by a three-dimensional magnetostatic model of the emergence
of a closed, spheroidal magnetic system in the corona, in which the
Lorentz force arising from cross-field currents is balanced by the
gravitational and pressure forces. This theoretical model carries many
features in common with the observed morphology of our active region.