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Waves in the Magnetized Solar Atmosphere. II. Waves from Localized Sources in Magnetic Flux Concentrations

Thomas J. BogdanNational Science Foundation, Arlington, VA 22203; and E. O. Hulbert Center for Space Research, Naval Research Laboratory, 4555 Overlook Avenue, SW, Washington, DC 20375Marie HansteenInstitute of Theoretical Astrophysics, University of Oslo, P.O. Box 1029, Blindern, Oslo, N-0315, NorwayA. D. McMurryInstitute of Theoretical Astrophysics, University of Oslo, P.O. Box 1029, Blindern, Oslo, N-0315, NorwayC. S. RosenthalCurrent address: Soskraenten 58, DK-8260 Viby J, DenmarkMichael D. JohnsonEvergreen State College, Olympia, WA 98505S. Petty‐PowellEvergreen State College, Olympia, WA 98505E. J. ZitaEvergreen State College, Olympia, WA 98505R. F. SteinDepartment of Physics and Astronomy, Michigan State University, East Lansing, MI 48824-1116Scott W. McIntoshLaboratory for Astronomy and Solar Physics, NASA Goddard Space Flight Center, Greenbelt, MD 20771; and Universities Space Research Association, CPSS, Seabrook, MD 20770Åke NordlundNiels Bohr Institute for Astronomy, Physics and Geophysics, Københavns Universitet, Blegdamsveg 17, Copenhagen Ø, DK-2100, Denmark
2003en
ABI

Аннотация

Numerical simulations of wave propagation in a two-dimensional stratified magneto-atmosphere are presented for conditions that are representative of the solar photosphere and chromosphere. Both the emergent magnetic flux and the extent of the wave source are spatially localized at the lower photospheric boundary of the simulation. The calculations show that the coupling between the fast and slow magnetoacoustic-gravity (MAG) waves is confined to thin quasi–one-dimensional atmospheric layers where the sound speed and the Alfvén velocity are comparable in magnitude. Away from this wave conversion zone, which we call the magnetic canopy, the two MAG waves are effectively decoupled because either the magnetic pressure (B 2 =8) or the plasma pressure (p NkBT) dominates over the other. The character of the fluctuations observed in the magneto-atmosphere depend sensitively on the relative location and orientation of the magnetic canopy with respect to the wave source and the observation point. Several distinct wave trains may converge on and simultaneously pass through a given location. Their coherent superposition presents a bewildering variety of Doppler and intensity time series because (1) some waves come directly from

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