1993
DOI: 10.1093/mnras/265.3.588
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The opacity mechanism in B-type stars - II. Excitation of high-order g-modes in main-sequence stars

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Cited by 221 publications
(180 citation statements)
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“…Secondly, only high-order g-modes (with long periods) can be excited, for low-order g-modes are affected by significant radiative damping. The same phenomenon occurs in SPB stars (Dziembowski et al 1993;Dupret et al 2008). Interestingly, the blue edge of the l ≤ 3 instability strip of our sdB models with OP opacities corresponds to the observed blue edge of the V1093 Her variables at log T eff = 4.47.…”
Section: Stability Analysis Of a Grid Of Sdb Modelssupporting
confidence: 81%
“…Secondly, only high-order g-modes (with long periods) can be excited, for low-order g-modes are affected by significant radiative damping. The same phenomenon occurs in SPB stars (Dziembowski et al 1993;Dupret et al 2008). Interestingly, the blue edge of the l ≤ 3 instability strip of our sdB models with OP opacities corresponds to the observed blue edge of the V1093 Her variables at log T eff = 4.47.…”
Section: Stability Analysis Of a Grid Of Sdb Modelssupporting
confidence: 81%
“…This is well justified because the pulsational instability mechanism and theoretical oscillation spectra of B stars were already reviewed by Dziembowski & Pamyatnykh (1992), Gautsschy & Saio (1993), Dziembowski et al (1993), Moskalik (1995), Dupret (2001), and others. More recent investigations (e.g.…”
Section: Oscillation Spectra Of Early-type Starsmentioning
confidence: 84%
“…The properties of the basic eigenfunctions, kinetic energy distributions and work integrals for models of B stars were already discussed by Dziembowski & Pamyatnykh (1992), Dziembowski et al (1993), Pamyatnykh (1999), Dziembowski (2009), Dupret (2001, and others. The proper behavior of the Rosseland-mean opacity and eigenfunctions are necessary, but not sufficient conditions for the κ-mechanism to work.…”
Section: Seismic Modelsmentioning
confidence: 90%
“…The observational properties of the SPB stars were broadly discussed, e.g., by Balona (2000) and , 2007. These modes are driven by the classical κ-mechanism operating in the metal opacity bump (Dziembowski, Moskalik & Pamyatnykh 1993;Gautschy & Saio 1993). There are three basic problems which complicate the interpretation of the SPB pulsations and make seismic modelling of these pulsators particularly difficult.…”
Section: Introductionmentioning
confidence: 99%