1999
DOI: 10.1086/311915
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Seismic Images of a Solar Flare

Abstract: We have used helioseismic holography to render seismic images of the solar flare of 1996 July 9, whose helioseismic signature was recently reported by Kosovichev & Zharkova. We computed time series of "egression power maps" in 2 mHz bands centered at 3.5 and 6 mHz. These images suggest an oblong acoustic source associated with the flare some 18 Mm in the north-south direction and approximately 15 Mm in the east-west direction. The considerable preponderance of the flare acoustic power emanates in the 3.5 mHz b… Show more

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Cited by 94 publications
(114 citation statements)
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“…The radiant points of the waves closely match the various signatures of the impulsive phase (Fig. 14;Lindsey and Donea 2008), and the optimum frequency bands for the holographic technique (Lindsey and Braun 1990;Donea et al 1999) appear to be 3-7 mHz, corresponding to time scales (2πω) −1 of 10-50 s.…”
Section: Seismic Wavesmentioning
confidence: 54%
“…The radiant points of the waves closely match the various signatures of the impulsive phase (Fig. 14;Lindsey and Donea 2008), and the optimum frequency bands for the holographic technique (Lindsey and Braun 1990;Donea et al 1999) appear to be 3-7 mHz, corresponding to time scales (2πω) −1 of 10-50 s.…”
Section: Seismic Wavesmentioning
confidence: 54%
“…At this depth, a field strength of ≈ 80 kG is inferred from flux-tube emerging calculations (see e.g. D'Silva and Choudhuri, 1993;Caligari, Moreno-Insertis, and Schüssler, 1995). The Alfvén travel time for a change at the base to propagate to the surface (more accurately: the propagation time of a transverse tube wave) is then about five days.…”
Section: The Anchoring Problemmentioning
confidence: 93%
“…Quite clear, however, is the picture of flux emergence: the process by which a loop of flux rises from a horizontal layer of magnetic flux at the base of the convection zone to form an active region, as discussed briefly in Section 2.1.1. Simplified 1D calculations in the "thin tube" approximation (D'Silva and Choudhuri, 1993;Fan, Fisher, and McClymont, 1994;Caligari, Moreno-Insertis, and Schüssler, 1995) point to a field strength of about 10 5 G at the base of the convection zone. At this strength, agreement is reached with three independent key properties of active regions: i) the time scale of emergence (a few days), ii) the heliographic-latitude range of emergence, and iii) the tilt of active-region axes (e.g.…”
Section: The Issue Of Flux Emergencementioning
confidence: 97%
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“…13a), [90][91][92][93], or indirectly by calculating integrated acoustic emission [94][95][96]. Solar flares are sources of high-temperature plasma and strong hydrodynamic motions in the solar atmosphere.…”
Section: Magnetic Effects: Sunspot Oscillations and Acoustic Halosmentioning
confidence: 99%