1996
DOI: 10.1038/379235a0
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Downflows under sunspots detected by helioseismic tomography

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Cited by 181 publications
(131 citation statements)
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“…At layers shallower than about 4 Mm, the flows might start to change from downflows to upflows, when flux emerges, and then back to downflows after the active regions are established. The flow response to emerging flux agrees with numerical simulations of emerging flux tubes (Fan, 2001;Schüssler and Rempel, 2005) where upflows indicate the beginning of flux emergence and surface cooling due to adiabatic expansion leads to downflows along the emerged loops. The kinetic-helicity density at 127.5°-135.0°longitude as a function of latitude and depth.…”
Section: Large-scale Flows Around Active Regionssupporting
confidence: 74%
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“…At layers shallower than about 4 Mm, the flows might start to change from downflows to upflows, when flux emerges, and then back to downflows after the active regions are established. The flow response to emerging flux agrees with numerical simulations of emerging flux tubes (Fan, 2001;Schüssler and Rempel, 2005) where upflows indicate the beginning of flux emergence and surface cooling due to adiabatic expansion leads to downflows along the emerged loops. The kinetic-helicity density at 127.5°-135.0°longitude as a function of latitude and depth.…”
Section: Large-scale Flows Around Active Regionssupporting
confidence: 74%
“…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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“…After they reflect off the Alfvén wave speed gradient, the fast waves may re-enter the solar interior wave field. This could be problematic for helioseismology, since any phase changes produced by the "fast-to-Alfvén" mode conversion process would seriously compromise any inferences derived from helioseismic inversions of phase travel times (e.g., Duvall et al 1996;Kosovichev, Duvall & Scherrer 2000;Couvidat et al 2005), which would normally, but inaccurately, interpret such phase changes as "travel-time shifts" due to subsurface inhomogeneities alone.…”
Section: Introductionmentioning
confidence: 99%