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Submitted on 7 Sep 2005

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EVOLUTION OF GALACTIC FIELD Be STARS

Juan Zorec, Yves Fremat, Lydia Cidale

To cite this version:

Juan Zorec, Yves Fremat, Lydia Cidale. EVOLUTION OF GALACTIC FIELD Be STARS. Societe

Francaise d’Astronomie et d’Astrophysique, 2005, France. �hal-00008525�

(2)

ccsd-00008525, version 1 - 7 Sep 2005

SF2A 2005

F. Casoli, T. Contini, J.M. Hameury, and L. Pagani (eds)

EVOLUTION OF GALACTIC FIELD BE STARS

Zorec, J.

1

, Fr´emat, Y.

2

and Cidale, L.

3 3

Abstract. Galactic field Be stars were studied by taking into account the effects induced by the fast rotation on their fundamental parameters. Frac-tional ages τ /τMS (τMS= time spent in the MS) against stellar mass reveal

that: a) Be stars spread over the whole interval 0 < τ /τMS< 1; b) the Be

phenomenon in massive stars (M > 12M⊙) is present at smaller age ratios

than for less massive stars (M < 12M⊙); c) there is a lack of Be stars with

M < 7M⊙in the first half of the MS. Low mass fast rotators (M < 7M⊙),

called Bn stars, could be “becoming” Be stars.

1 Sample and Method

We studied 97 field galactic bright Be stars using the BCD system (Chalonge & Divan 1956, Zorec & Briot 1991) to avoid perturbations on the fundamental parameters due to the circumstellar disc. These parameters were treated for rota-tional effects (Fr´emat et al. 2005). From the observed parameters, called apparent, we obtain first the parent non-rotating counterparts (pnrc) which represent homo-logous stars without rotation. To enter the evolutionary tracks, we transform then the pnrc into averaged parameters over the whole stellar surface.

2 Results and Conclusions

Figure 1a) shows the distribution of points (τ /τMS, M/M⊙) obtained using the

original or apparent fundamental parameters and the evolutionary tracks without rotation (Schaller et al. 1992). The plotted error bars correspond to measurement uncertainties. Figure 1b) shows the same type of distribution, but where

param-eters were corrected for rotational effects assuming rigid rotation with Ω/Ωcrit=

0.9 (Fr´emat et al. 2005) and models of stellar evolution with rotation calculated by

Meynet & Maeder (2000) with ZAMS equatorial velocity VZAMS= 300 km s−1. In

both diagrams of Fig. 1, points spread over the whole interval of age fractions 0∼<

1Institut d’Astrophysique de Paris, UMR7095 CNRS, Universit´e Pierre & Marie Curie 2Royal Observatory of Belgium

3Facultad de Ciencias Astron´omicas y Geof´ısicas, Universidad de La Plata, Argentina

c

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2 SF2A 2005

τ /τMS

<

∼ 1, which suggest that the Be phenomenon may appear at whatever stage of the stellar evolution on the MS evolution phase. There is, however, a difference between the diagrams where rotation is taken into account and where it is not. If we were not aware of rotational effects, Fig. 1a would suggest that 86% of stars

are above the τ /τMS = 0.5 limit. Figure 1b shows, however, when fast rotation

of Be stars is taken into account, the fraction of stars in our sample above τ ≃

0.5τMS slumps to 62%. When we separate the stars into massive (M

>

∼ 12M⊙)

and less massive ones (M ∼ 12M< ⊙) another important result appears: we see in

Fig. 1b that the Be phenomenon in massive stars tends to appear on average at

smaller τ /τMS age fractions than in the less massive stars. There is also a striking

lack of low-mass Be stars (M ∼ 7M< ⊙) in τ /τMS < 1/2. These distributions can

be due to: i) higher mass-loss rates in massive objects, which reduce the surface fast rotation and inhibit the Be phenomenon rapidly; ii) circulation time scales to transport angular momentum from the core to the surface, which are longer the lower the stellar mass. Some of low-mass fast rotators, classified as Bn stars, could then be “becoming” Be stars.

30 25 20 15 10 5 0 M/M 0.0 0.2 0.4 0.6 0.8 1.0 /MS ... ... ... ... ... ZAMS TAMS / c= 0.00 a) 30 25 20 15 10 5 0 M/M 0.0 0.2 0.4 0.6 0.8 1.0 /MS ... ... ... ... ... ZAMS TAMS / c= 0.88 b)

Fig. 1.Age ratios τ /τMSof the studied Be stars against the mass. a) Parameters derived

using evolutionary tracks without rotation; b) parameters derived using evolutionary tracks with rotation

References

Chalonge, D., & Divan, L. 1952, Ann. Astrophys., 15, 201 Meynet, G., Maeder. A. 2000, A&A, 361, 101

Fr´emat, Y., Zorec, J., Hubert, A.M., Floquet, M. 2005, A&A, 440, 305 Schaller G., Schaerer D., Meynet G. et al. 1992, A&AS 96, 269 Zorec J., & Briot D., 1991, A&A 245, 150

Figure

Fig. 1. Age ratios τ /τ MS of the studied Be stars against the mass. a) Parameters derived using evolutionary tracks without rotation; b) parameters derived using evolutionary tracks with rotation

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