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1996
DOI: 10.1086/177429
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Absorption of p-Modes by Slender Magnetic Flux Tubes and p-Mode Lifetimes

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Cited by 74 publications
(111 citation statements)
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“…Unfortunately with observations at a single height they were unable to identify what mixture of m = 0, axisymmetric sausage-modes, and m = 1, kinkmodes, they were observing. Theoretical studies of the interaction of flux tubes and waves have been performed in the past, for example Roberts and Webb (1979), Wilson (1980), Spruit (1981), Spruit (1982), Bogdan and Knölker (1989), Solanki (1993), Bogdan et al (1996), Hasan and Kalkofen (1999), Tirry (2000), Gizon, Hanasoge, and Birch (2006), Jain and Gordovskyy (2008), Hanasoge et al (2008), Hanasoge and Cally (2009). It is now well established that slender magnetic flux tubes permit the propagation of the two basic types of magnetohydrodynamic waves: The longitudinal tube waves (sausage modes) with azimuthal wave number m = 0, which are axisymmetric, excited by pressure fluctuations.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately with observations at a single height they were unable to identify what mixture of m = 0, axisymmetric sausage-modes, and m = 1, kinkmodes, they were observing. Theoretical studies of the interaction of flux tubes and waves have been performed in the past, for example Roberts and Webb (1979), Wilson (1980), Spruit (1981), Spruit (1982), Bogdan and Knölker (1989), Solanki (1993), Bogdan et al (1996), Hasan and Kalkofen (1999), Tirry (2000), Gizon, Hanasoge, and Birch (2006), Jain and Gordovskyy (2008), Hanasoge et al (2008), Hanasoge and Cally (2009). It is now well established that slender magnetic flux tubes permit the propagation of the two basic types of magnetohydrodynamic waves: The longitudinal tube waves (sausage modes) with azimuthal wave number m = 0, which are axisymmetric, excited by pressure fluctuations.…”
Section: Introductionmentioning
confidence: 99%
“…The pressure, density and sound speed vary as power laws (see Bogdan et al 1996 for details). Following Bogdan et al (1996), Hindman & Jain (2008) and Jain et al (2009) we set the truncation depth at z = −z 0 352 A. Gascoyne & R. Jain which is our model photosphere where the quantities ρ 0 and P 0 are the values of the mass density and gas pressure at this depth. Above the truncation depth z > −z 0 we assume the existence of a hot vacuum (ρ ext → 0 with temperature T ext → ∞).…”
Section: Equilibrium Configurationmentioning
confidence: 99%
“…For these thin magnetic flux tubes, the lateral variation of the magnetic field across the tube is ignored and the plasma β is constant with depth (see Bogdan et al 1996 andJain 2008 for details).…”
Section: Equilibrium Configurationmentioning
confidence: 99%
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