2000
DOI: 10.1017/s0252921100055536
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Physical Properties and Evolutionary Stage of Be Stars

Abstract: The determination of accurate and reliable basic physical properties of Be stars is a very complicated task which, among other things, requires a good knowledge of the variability pattern of each particular object. Possible confusion between a rotationally distorted photosphere and a pseudophotosphere – an inner optically thick part of a gradually formed envelope which temporarily mimics a photosphere – is discussed in some detail in relation to the stellar effective temperature, brightness and rate of rotatio… Show more

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Cited by 50 publications
(69 citation statements)
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“…HR 1910ζ Tau. This is a long known single-line spectroscopic binary CBe (Harmanec 1984;Ruždjak et al 2009). The nature of the companion has not been confirmed and the possibilities include a rather cool sdOB or a late-type main sequence companion (Schaefer et al 2010).…”
Section: A Known Binaries In the Samplementioning
confidence: 99%
“…HR 1910ζ Tau. This is a long known single-line spectroscopic binary CBe (Harmanec 1984;Ruždjak et al 2009). The nature of the companion has not been confirmed and the possibilities include a rather cool sdOB or a late-type main sequence companion (Schaefer et al 2010).…”
Section: A Known Binaries In the Samplementioning
confidence: 99%
“…(a) Slettebak (1982); (b) Rivinius et al (2006); (c) Harmanec (1988); (d) van Leeuwen (2007) modeled as a combination of a fast-rotating central star surrounded by a VDD. The code uses the Monte Carlo method to solve the radiative transfer, radiative equilibrium, and statistical equilibrium in 3D geometry for the given density and velocity distributions for pure hydrogen gas.…”
Section: Modeling Proceduresmentioning
confidence: 99%
“…Mass and radius determination for κ CMa from the Harmanec (1988) compilation for the effective temperatures given by Popper (1980), Prinja (1989) and Fremat (2005 (4.98 -6.36) effective temperatures used by Popper (1980), Prinja (1989) and Fremat (2005), we obtain the Table 1. Thus, for a main sequence star the stellar radius should be smaller than the 6 R we have adopted, however, our radius estimate based on the parallax and the chosen V magnitude from the correlation between the brightness and emission strength, as proposed by Harmanec (2000), gives the range of radii comparable to the 6 R used in our modeling.…”
Section: Introductionmentioning
confidence: 96%