The initiation of coronal mass ejections by newly emerging magnetic flux

We present observational evidence that eruptions of quiescent filaments and associated coronal mass ejections (CMEs) occur as a consequence of the destabilization of large-scale coronal arcades due to interactions between these structures and new and growing active regions. Both statistical and case studies have been carried out. In a case study of a 'bulge' observed by the High-Altitude Observatory Solar Maximum Mission coronagraph, the high-resolution magnetograms from the Big Bear Solar Observatory show newly emerging and rapidly changing flux in the magnetic fields that apparently underlie the bugle. For other case studies and in the statistical work the eruption of major quiescent filaments was taken as a proxy for CME eruption. We have found that two thirds of the quiescent-filament-associated CMEs occurred after substantial amounts of new magnetic flux emerged in the vicinity of the filament. In addition, in a study of all major quiescent filaments and active regions appearing in a 2-month period we found that 17 of the 22 filaments that were associated with new active regions erupted and 26 of the 31 filaments that were not associated with new flux did not erupt. In all cases in which the new flux was oriented favorably for reconnection with the preexisting large-scale coronal arcades; the filament was observed to erupt. The appearance of the new flux in the form of new active regions begins a few days before the eruption and typically is still occurring at the time of the eruption. A CME initiation scenario taking account of these observational results is proposed.

[1]  A. Hundhausen,et al.  Coronal mass ejections and major solar flares: The great active center of March 1989 , 1994 .

[2]  O. C. St. Cyr,et al.  Speeds of coronal mass ejections: SMM observations from 1980 and 1984‐1989 , 1994 .

[3]  J. Gosling The solar flare myth , 1993 .

[4]  A. Hundhausen,et al.  Sizes and locations of coronal mass ejections - SMM observations from 1980 and 1984-1989 , 1993 .

[5]  B. Low,et al.  The free energies of partially open coronal magnetic fields , 1993 .

[6]  C. Cyr,et al.  A Revised and Expanded Catalogue of Mass Ejections Observed by the Solar Maximum Mission Coronagraph , 1993 .

[7]  R. S. Steinolfson Three-dimensional structure of coronal mass ejections , 1992 .

[8]  S. Wu,et al.  A numerical simulation of magnetically driven coronal mass ejections , 1992 .

[9]  D. Rust,et al.  Variation of the vector magnetic field in an eruptive flare , 1992 .

[10]  D. Webb The solar sources of coronal mass ejections , 1992 .

[11]  S. Nozawa,et al.  Magnetic Reconnection Associated with Emerging Magnetic Flux , 1992 .

[12]  D. Webb,et al.  Activity associated with coronal mass ejections at solar minimum: SMM observations from 1984–1986 , 1991 .

[13]  S. Martin Elementary bipoles of active regions and ephemeral active regions , 1991 .

[14]  A. Hundhausen,et al.  The launch of solar coronal mass ejections: Results from the coronal mass ejection onset program , 1990 .

[15]  B. Low EQUILIBRIUM AND DYNAMICS OF CORONAL MAGNETIC FIELDS , 1990 .

[16]  A. Hundhausen,et al.  Density and white light brightness in looplike coronal mass ejections: Temporal evolution , 1988 .

[17]  J. Cook,et al.  Plasma motions in an emerging flux region , 1988 .

[18]  S. Kahler Coronal mass ejections , 1987 .

[19]  A. Hundhausen,et al.  Activity associated with the solar origin of coronal mass ejections , 1987 .

[20]  A. Hundhausen The Origin and Propagation of Coronal Mass Ejections (R) , 1987 .

[21]  R. Harrison Solar coronal mass ejections and flares , 1986 .

[22]  K. L. Harvey,et al.  Relationships of a growing magnetic flux region to flares , 1984 .

[23]  R. MacQueen,et al.  The kinematics of solar inner coronal transients , 1983 .

[24]  E. Priest,et al.  A numerical experiment relevant to line-tied reconnection in two-ribbon flares , 1983 .

[25]  E. Hildner,et al.  Coronal Observations from the Solar Maximum Mission Satellite , 1982 .

[26]  U. Anzer,et al.  Magnetic reconnection and coronal transients , 1982 .

[27]  R. Wolfson Equilibria and stability of coronal magnetic arches , 1982 .

[28]  B. Low,et al.  The initiation of a coronal transient , 1982 .

[29]  K. L. Harvey,et al.  Emerging magnetic flux, flares and filaments - FBS interval 16-23 June 1980 , 1982 .

[30]  P. McIntosh,et al.  Disappearing solar filaments: A useful predictor of geomagnetic activity , 1981 .

[31]  P. Seagraves,et al.  On the coronal transient-eruptive prominence of 1980 August 5 , 1981 .

[32]  C. Sawyer,et al.  Studies of the corona with the Solar Maximum Mission coronagraph/polarimeter , 1981 .

[33]  K. Sheridan,et al.  Radio and visible light observations of matter ejected from the sun , 1981 .

[34]  B. Labonte,et al.  Observational Search for Variations in the Solar Convection , 1980 .

[35]  E. Hildner,et al.  The High Altitude Observatory Coronagraph/Polarimeter on the Solar Maximum Mission , 1980 .

[36]  R. MacQueen,et al.  The association of coronal mass ejection transients with other forms of solar activity , 1979 .

[37]  E. Priest,et al.  Thermal evolution of current sheets and flash phase of solar flares , 1976 .

[38]  D. Rust An active role for magnetic fields in solar flares , 1976 .

[39]  J. D. Bohlin,et al.  Coronal changes associated with a disappearing filament , 1975 .

[40]  V. Grigorjev,et al.  Magnetoactive lines in the medium with the velocity gradient , 1975 .

[41]  R. MacQueen,et al.  Mass ejections from the Sun: A view from Skylab , 1974 .

[42]  A. Hundhausen,et al.  Observation of a solar flare induced interplanetary shock and helium-enriched driver gas , 1970 .

[43]  D. Colburn,et al.  Interplanetary field and geomagnetic variations a unified view , 1969 .

[44]  F. A. Lindemann LXX. Note on the theory of magnetic storms , 1919 .

[45]  R. Hodgson,et al.  On a curious Appearance seen in the Sun , 1859 .

[46]  R. C. Carrington Description of a Singular Appearance seen in the Sun on September 1, 1859 , 1859 .