Formation of a Solar Filament Channel

We present observations of the early stages of formation of a filament channel when a compact activity complex emerged in a previously quiet, near-equatorial area. In a few hours, and while flux was rising rapidly in one bipolar component in the complex, Hα fine structure overlying a polarity inversion zone organized into a conspicuous pattern of parallel fibrils enclosing the trailing end of the new activity complex. Yet it took another 4 days for a stable filament to form inside that pattern. It did so at a place where migrating positive polarity flux from the new activity complex contacted the negative polarity flux in a plage of an adjacent decaying bipolar active region. In contrast, no filament formed along an existing channel inside the adjacent decaying region; the opposite-polarity fluxes on the borders of the existing channel showed no signs of convergence. We attribute the fibril-aligning forces in the new channel to the horizontal component of an extended nonpotential magnetic field caused by currents in the multipolar activity complex. The channel is, in this view, an elementary part of the magnetic topology of an activity complex. We propose that the later formation of the filament in the new channel requires an additional and separate process. A plausible candidate for this second step is the development of a current sheet at the site of converging magnetic flux.

[1]  B. Low Three-dimensional structures of magnetostatic atmospheres. IV: Magnetic structures over a solar active region , 1992 .

[2]  S. Martin Conditions for the formation of prominences as inferred from optical observations , 1990 .

[3]  P. Foukal Morphological relationships in the chromospheric Hα fine structure , 1971 .

[4]  N. Sheeley,et al.  The rotation of photospheric magnetic fields: A random walk transport model , 1994 .

[5]  K. L. Harvey,et al.  Observations of moving magnetic features near sunspots , 1973 .

[6]  S. Martin,et al.  Magnetic Field Configurations Basic to Filament Channels and Filaments , 1993 .

[7]  V. Gaizauskas,et al.  Interactions between nested sunspots. 1: The formation and breakup of a delta-type sunspot , 1994 .

[8]  David M. Rust,et al.  Helical magnetic fields in filaments , 1994 .

[9]  Petrus C. H. Martens,et al.  Formation and eruption of solar prominences , 1989 .

[10]  F. Tang Quiescent prominences - where are they formed? , 1987 .

[11]  John Warren Harvey,et al.  Large-scale patterns formed by solar active regions during the ascending phase of cycle 21 , 1983 .

[12]  T. Yeh Polarity neutral lines on the solar surface and magnetic structures in the corona , 1987 .

[13]  J. Feynman,et al.  The initiation of coronal mass ejections by newly emerging magnetic flux , 1995 .

[14]  D. Vrabec Magnetic Field Spectroheliograms from the San Fernando Observatory , 1971 .

[15]  P. McIntosh,et al.  Solar magnetic fields derived from hydrogen alpha filtergrams , 1972 .