1982
DOI: 10.1086/159736
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Resonant electrodynamic heating of stellar coronal loops - an LRC circuit analog

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Cited by 146 publications
(43 citation statements)
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“…For these low frequencies, the transition region (T.R.) acts as a transmitting and reflecting barrier, with the important property that the transmission is not symmetric, so that a coronal loop acts as a cavity that resonates at specific frequencies, based on the Alfvén crossing time t with n = 0, 1... (Ionson 1982;Hollweg 1984).…”
Section: Introductionmentioning
confidence: 99%
“…For these low frequencies, the transition region (T.R.) acts as a transmitting and reflecting barrier, with the important property that the transmission is not symmetric, so that a coronal loop acts as a cavity that resonates at specific frequencies, based on the Alfvén crossing time t with n = 0, 1... (Ionson 1982;Hollweg 1984).…”
Section: Introductionmentioning
confidence: 99%
“…The departure to inhomogeneity typically introduces a variety of phenomena such as resonant absorption (in the corona see, e.g., Ionson 1978Ionson , 1982Ionson , 1983Hollweg 1984;Ruderman & Roberts 2002) and phase mixing (e.g. Heyvaerts & Priest 1983), all of which blur the distinction between these separate modes (see also, e.g., Bogdan et al 2003;McDougall & Hood 2007;Sousa & Cunha 2008;Cally & Hansen 2011;Hansen & Cally 2012).…”
Section: Introductionmentioning
confidence: 99%
“…m , where a is the width of an elemental magnetic loop, Re m = v A a/η D is the magnetic Reynolds number, v A is the Alfvén velocity, and η D = c 2 /4πσ is magnetic diffusivity, with σ = 1.96 ne 2 /(m e ν ei ) being the plasma conductivity (Ionson 1982;Ryutova & Habbal 1995).…”
Section: Phenomenology and Quantitative Analysismentioning
confidence: 99%