2009
DOI: 10.1051/0004-6361/200810471
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Collective pulsational velocity broadening due to gravity modes as a physical explanation for macroturbulence in hot massive stars

Abstract: Aims. We aimed at finding a physical explanation for the occurrence of macroturbulence in the atmospheres of hot massive stars, a phenomenon found in observations for more than a decade but that remains unexplained. Methods. We computed time series of line profiles for evolved massive stars broadened by rotation and by hundreds of low-amplitude nonradial gravity-mode pulsations which are predicted to be excited for evolved massive stars. Results. In general, line profiles based on macrotubulent broadening can … Show more

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Cited by 140 publications
(218 citation statements)
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“…The five stars color coded in blue are bona fide γ Dor pulsators. Right: as in left panel, with overplotted the location of ≈300 γ Dor stars analyzed by Bruntt et al (2008), Catanzaro et al (2011), Fossati et al (2011), Tkachenko et al (2012, Bradley et al (2015), and Van Reeth et al (2015) and some hybrid γ Dor-δ Sct stars from Catanzaro et al (2011) and Tkachenko et al (2012). broadening of spectral lines (Aerts et al 2009). If indeed turbulent pressure fluctuations excite high-order modes, a connection with γ Dor may be present as well, which could involve finite amplitude pressure fluctuations in the HCZ.…”
Section: Discussionmentioning
confidence: 99%
“…The five stars color coded in blue are bona fide γ Dor pulsators. Right: as in left panel, with overplotted the location of ≈300 γ Dor stars analyzed by Bruntt et al (2008), Catanzaro et al (2011), Fossati et al (2011), Tkachenko et al (2012, Bradley et al (2015), and Van Reeth et al (2015) and some hybrid γ Dor-δ Sct stars from Catanzaro et al (2011) and Tkachenko et al (2012). broadening of spectral lines (Aerts et al 2009). If indeed turbulent pressure fluctuations excite high-order modes, a connection with γ Dor may be present as well, which could involve finite amplitude pressure fluctuations in the HCZ.…”
Section: Discussionmentioning
confidence: 99%
“…Indeed, oscillations change the shape of spectral lines in an asymmetric and time-dependent way, i.e., the level of deformation depends on the phase in the overall oscillation cycle. To compensate for this deformation and absence of pulsational broadening, one usually introduces a time-independent ad-hoc parameter called macroturbulence (e.g., Aerts et al 2009) and/or a rotational profile with a wrong v sin i, each of which are usually deduced from metal lines and have a different functional shape than the true time-dependent line-broadening function. This is then compensated for by an incorrect value of the gravity and/or microturbulence, which can either be too high or too low.…”
Section: Discussionmentioning
confidence: 99%
“…Cantiello et al (2009) evoke the subphotospheric convection to account for the microturbulent motions, while Aerts et al (2009Aerts et al ( , 2014 suggest that macro-turbulence could be ascribed to low-amplitude gravity modes of nonradial pulsations. Similar conclusions are also put forward by Simón-Díaz (2015).…”
Section: Preliminary Commentsmentioning
confidence: 99%