2023A&A...676A..81Z


Query : 2023A&A...676A..81Z

2023A&A...676A..81Z - Astronomy and Astrophysics, volume 676A81 (2023/8-1)

Study of a sample of faint Be stars in the exofield of CoRoT III. Global spectroscopic characterization and astrophysical parameters of the central stars.

ZOREC J., HUBERT A.M., MARTAYAN C. and FREMAT Y.

Abstract (from CDS):

Context. The search and interpretation of non-radial pulsations from Be star light curves observed with the CoRoT satellite requires high-quality stellar astrophysical parameters.
Aims. The present work is devoted to the spectroscopic study of a sample of faint Be stars observed by CoRoT in the fourth long run (LRA02).
Methods. The astrophysical parameters were determined from the spectra in the λλ4000-4500 Å wavelength domain observed with the VLT/FLAMES instruments at ESO. Spectra were fitted with models of stellar atmospheres using our GIRFIT package. Spectra obtained in the λλ6400-7200 Å wavelength domain enabled the confirmation or, otherwise, a first identification of Be star candidates.
Results. The apparent parameters (Teff, log g, Vsini) for a set of 19 B and Be stars were corrected for the effects induced by the rapid rotation. These allowed us to determine: (1) stellar masses that are in agreement with those measured for detached binary systems; (2) spectroscopic distances that agree with the Gaia parallaxes; and (3) centrifugal/gravity equatorial force ratios of ∼0.6-0.7, which indicate that our Be stars are subcritical rotators. A study of the Balmer Hα, Hγ and Hδ emission lines produced: (1) extents of the circumstellar disk (CD) emitting regions that agree with the interferometric inferences in other Be stars; (2) R- dependent exponents n(R) = ln[ρ(R)/ρo]/ln(Ro/R) of the CD radial density distributions; and (3) CD base densities ρo similar to those inferred in other recent works.
Conclusions. The Hγ and Hδ emission lines are formed in CD layers close to the central star. These lines produced a different value of the exponent n(R) than assumed for Hα. Further detailed studies of Hγ and Hδ emission lines could reveal the physical properties of regions where the viscous transport of angular momentum to the remaining CD regions is likely to originate from. The subcritical rotation of Be stars suggests that their huge discrete mass-ejections and concomitant non-radial pulsations might have a common origin in stellar envelope regions that become unstable to convection due to rotation. If it is proven that the studied Be stars are products of binary mass transfer phases, the errors induced on the estimated Teff by the presence of stripped sub-dwarf O/B companions are not likely to exceed their present uncertainties.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: early-type - stars: emission-line - Be - stars: fundamental parameters - stars: oscillations

VizieR on-line data: <Available at CDS (J/A+A/676/A81): tabled1.dat tabled2.dat>

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 HD 49330 bC* 06 47 57.2679459720 +00 46 34.035384504 8.45 9.14 8.95     Bnn(e) 98 0
4 CoRoT 300002611 * 06 48 19.6847643992 -03 43 27.388256949           ~ 1 0
5 CoRoT 300002834 * 06 48 25.8625230687 -03 26 21.135622345           ~ 1 0
6 CoRoT 300003290 * 06 48 36.9035966249 -03 53 45.792642381           ~ 1 0
7 CoRoT 110827583 V* 06 48 58.5343461528 -05 13 06.254681412   16.025 15.331 15.132   ~ 2 0
8 CoRoT 110655185 V* 06 49 06.0951170856 -05 00 21.863674476   16.470 15.670 15.514   ~ 2 0
9 CoRoT 110655384 V* 06 49 06.7996656984 -05 20 41.770838904   16.714 16.073 15.943   ~ 2 0
10 CoRoT 110655437 EB* 06 49 06.9770641800 -05 02 27.302448012     16.030 15.757   ~ 3 0
11 UCAC4 434-022818 Pu* 06 50 10.7310537576 -03 20 55.791697020   14.81 14.11 13.93   B3V 3 0
12 CoRoT 110663174 V* 06 50 11.9408056968 -04 40 53.216649336   17.244 16.464 16.147   ~ 2 0
13 UCAC4 434-022837 gD* 06 50 14.3618933928 -03 23 59.503300404   15.49 14.51 14.30   B8Ia 3 0
14 CoRoT 110747131 V* 06 50 27.0412323264 -05 26 36.856095828   15.010 14.180 14.717   ~ 4 0
15 UCAC4 434-022958 V* 06 50 39.0911719584 -03 18 14.368218732   13.73 13.268 13.24   B8V 3 0
16 CoRoT 110672515 Pu* 06 51 14.2419215424 -05 23 51.024911028   16.971 16.062 15.422   ~ 2 0
17 TYC 4808-1005-1 Em* 06 51 17.5117225680 -04 36 59.966547300   11.58 11.40 11.47   B5III 6 0
18 EM* AS 136 Pu* 06 51 17.5237888248 -03 19 29.711604504 11.21 11.83 11.48     B 13 0
19 [KER2009] lra2a 1163 RR* 06 51 18.1945308720 -04 07 40.617645744     15.875     ~ 3 0
20 UCAC4 434-023239 V* 06 51 23.7950024928 -03 14 46.509056736   14.01 13.55 13.45   B7II 3 0
21 TYC 4804-115-1 V* 06 52 08.3230436472 -03 37 52.330300644   12.33 11.86 12.07   B8V 5 0
22 TYC 4809-1869-1 Pu* 06 53 00.9392789952 -04 40 18.173757360   11.38 11.31 11.42   B6III 5 0
23 * ome CMa Be* 07 14 48.6540133346 -26 46 21.603204215 2.90 3.64 3.82 3.80 3.90 B2.5Ve 373 0
24 * 66 Oph Be* 18 00 15.7957050537 +04 22 07.122326765 3.77 4.58 4.60 4.47 4.49 B2Ve 358 0

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