1999A&A...349..151M


Query : 1999A&A...349..151M

1999A&A...349..151M - Astronomy and Astrophysics, volume 349151-168 (1999/9-1)

Long-term visual spectrophotometric behaviour of Be stars. II. Correlations with fundamental stellar parameters and interpretation.

MOUJTAHID A., ZOREC J. and HUBERT A.M.

Abstract (from CDS):

The long-term visual spectrophotometric (SPh) behaviour of Be stars as a function of fundamental stellar parameters is studied. Some previous SPh results obtained by other authors are confirmed. Moreover, a tendency for temperature and aspect angle dependency of SPh variations is found. From the characteristics of visual SPh behaviour in Be stars we derive constraints for models of regions in circumstellar envelopes where the visual continuum spectrum is formed: (i) The SPh emission and absorption phases should not imply preferential aspect angles, as they can both appear whatever the stellar inclination. This phenomenon cannot be always accounted for by strongly flattened circumstellar envelopes; (ii) Radii of the visible continuum forming regions cannot be larger than a few R*; (iii) Electron densities of these regions should not exceed Ne∼1013cm–3; (iv) Electron temperature of circumstellar layers producing the SPh emission phases compare with the stellar Balmer continuum radiation temperature and it is much lower in those producing the SPh absorption phases. Three scenarios were studied to produce the observed characteristics of emissions in the V magnitude and in the second component of Balmer discontinuity (ΔD) during the SPh emission phases: (a) expansion of a massive circumstellar shell that preserves circumstellar envelope flattening; (b) expansion of a circumstellar shell which increases the global flattening, so that a disc-like structure is formed; (c) continuous mass ejection that increases the storage of mass in a constant volume with a given flattening. Mechanisms (a) and (b) produce a double valued (ΔV,ΔD) SPh relation, while (c) produces a single valued relation. Only mechanisms (a) and (c) can easily produce the observed amounts of emission ΔV and ΔD without violating the modeling constraints from (i) to (iv) imposed by observations. The model SPh slopes of (ΔV,ΔD) show the global sin i and Teff observed dependencies. The scenarios used to describe the double valued (ΔV,ΔD) suggest another possible way how to build up circumstellar envelopes around Be stars.

Abstract Copyright: ∼

Journal keyword(s): stars: activity - stars: atmospheres - stars: circumstellar matter - stars: emission-line, Be

Simbad objects: 48

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Number of rows : 48
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 * omi Cas Be* 00 44 43.5186007265 +48 17 03.731037403 3.91 4.44 4.50 4.45 4.50 B5IIIe 291 0
2 * gam Cas HXB 00 56 42.5310945 +60 43 00.264089 1.18 2.29 2.39 2.32 2.40 B0.5IVpe 1253 0
3 * 28 Tau Be* 03 49 11.2165977912 +24 08 12.156712008 4.73 5.01 5.09   5.08 B8Vne 494 0
4 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 1037 0
5 * c Per Be* 04 08 39.6935695869 +47 42 45.038007366 3.45 4.00 4.03 3.91 3.93 B3Ve 394 0
6 * 228 Eri Be* 04 29 06.9254098152 -13 02 54.127769208 4.45 5.23 5.41 5.46 5.63 B2(V)ne 286 0
7 * 11 Cam Be* 05 06 08.4527318736 +58 58 20.543222820 4.31 5.00 5.08     B3Ve 221 0
8 * lam Eri Be* 05 09 08.7840557047 -08 45 14.701594805 3.17 4.07 4.27 4.35 4.55 B2III(e)p 316 1
9 * psi01 Ori Be* 05 24 44.8273848312 +01 50 47.201915688 3.83 4.76 4.96 5.04 5.26 B1Vn 372 0
10 * zet Tau Be* 05 37 38.6854231 +21 08 33.158804 2.22 2.84 3.03 3.06 3.15 B1IVe_shell 751 0
11 HD 37967 Be* 05 43 19.5024321168 +23 12 15.748208100 5.51 6.15 6.21     B4Ve 112 0
12 * 10 CMa Be* 06 44 28.4671043496 -31 04 13.892357820 4.18 5.08 5.17 5.15 5.17 B2V 150 0
13 V* V505 Mon SB* 06 45 49.9771800456 +02 29 57.397214904 6.85 7.16 7.22     B6Ib 64 0
14 V* HZ CMa Be* 06 50 23.3482557912 -31 42 21.808309320   5.829 5.747     B6IVe+A 96 0
15 * 27 CMa Be* 07 14 15.2117197408 -26 21 09.028965559 3.76 4.45 4.65 4.64 4.73 B4Ve_sh 240 0
16 * 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
17 HD 58050 Be* 07 24 27.6487438296 +15 31 01.908288624 5.39 6.23 6.41     B2Ve 138 0
18 HD 58978 Be* 07 26 59.4826856664 -23 05 09.689679528 4.51 5.45 5.56 7.05   B0.5IVe 248 0
19 HD 60855 Be* 07 36 03.8931067344 -14 29 33.978895368 4.87 5.58 5.70 5.72 5.81 B2Ve 160 0
20 HD 60848 Be* 07 37 05.7325392528 +16 54 15.300327852 5.55 6.67 6.87     O8:V:pe 150 0
21 * omi Pup Be* 07 48 05.1686329933 -25 56 13.810593657 3.42 4.43 4.49 4.37 4.37 B1IVe 228 0
22 HD 65875 Be* 08 00 44.1338106480 -02 52 54.913100736 5.68 6.49 6.59 6.48 6.50 B2.5Ve 143 0
23 * r Pup Be* 08 13 29.5172754003 -35 53 58.265647773 3.68 4.66 4.77 4.68 4.77 B1V 199 0
24 * I Hya Be* 09 41 17.0067101149 -23 35 29.451517089 4.07 4.65 4.76 4.75 4.84 B5V 182 0
25 * J Vel Be* 10 20 54.7957129824 -56 02 35.655748188 3.80 4.38 4.51 6.02   B5II 112 0
26 HD 91120 Be* 10 30 59.8371178656 -13 35 18.495281472 5.38 5.54 5.58     B9IIIe 111 0
27 * p Car Be* 10 32 01.4650915230 -61 41 07.195030368 2.46 3.18 3.27 3.22 3.28 B4Vne 243 0
28 * kap Dra Be* 12 33 28.9433168544 +69 47 17.659892220 3.18 3.75 3.89 3.84 3.92 B6IIIe 395 0
29 HD 120991 Be* 13 53 57.2397645360 -47 07 41.390612184 5.11 6.03 6.10 6.24 6.34 B2Ve 145 0
30 * tet Cir Be* 14 56 43.9850523987 -62 46 51.675365388 4.34 5.11 5.11 4.87 4.79 B2III 120 0
31 * 48 Lib Be* 15 58 11.3682502453 -14 16 45.681109093 4.61 4.77 4.87 4.91 4.96 B5IIIp_sh 446 0
32 * chi Oph Be* 16 27 01.4355697915 -18 27 22.499961252 3.95 4.71 4.43 3.97 3.73 B2Vne 624 0
33 HD 162428 Be* 17 50 01.2322158096 +24 28 05.086357032   7.016 7.098     B7IV/Vn(e)_(sh) 44 0
34 * z Her Be* 17 50 03.3345672768 +48 23 38.948985636 6.380 6.790 6.890     B6IIInp_sh 168 0
35 HD 168797 Be* 18 21 28.4010720600 +05 26 08.560470876 5.47 6.09 6.13     B2Vne 127 0
36 HD 173219 Be* 18 44 33.3405747264 -07 06 38.163359880 7.26 8.00 7.88     B1:V:npe 88 0
37 HD 178175 Be* 19 08 16.7018664360 -19 17 25.037957508 4.79 5.43 5.49 5.50 5.51 B2Ve 150 0
38 HD 183656 Be* 19 30 33.1219108488 +03 26 39.860267784 5.69 6.064 6.082     B7III 133 0
39 HD 184279 Be* 19 33 36.9185843448 +03 45 40.793081472 6.63 7.00 7.00     B0V 153 0
40 * 12 Vul Be* 19 51 04.1083085616 +22 36 36.172997964 4.15 4.84 4.96 4.98 5.12 B2.5Ve 192 0
41 * b02 Cyg Be* 20 09 25.6190611128 +36 50 22.633958400 4.03 4.80 4.93     B2.5Ve 281 0
42 * 1 Del ** 20 30 17.96064 +10 53 45.3233 5.94 6.05 6.08     A1:III 109 0
43 * f01 Cyg Be* 20 59 49.5541247496 +47 31 15.363746436 3.77 4.71 4.75 4.62 4.63 B1.5Vnne 514 0
44 * eps Cap Be* 21 37 04.8311169408 -19 27 57.640399810 3.69 4.35 4.55 4.60 4.74 B3V 266 0
45 * 25 Peg Be* 22 07 50.3038755192 +21 42 10.536282684 5.27 5.68 5.78     B7Vne 119 0
46 HD 217050 Be* 22 57 04.5020619144 +48 41 02.645623680 4.81 5.34 5.43     B4IIIpe 340 1
47 HD 217543 Be* 23 00 54.7485457920 +38 42 28.238625504 5.78 6.43 6.54     B2.5Vn 109 0
48 HD 218674 Be* 23 09 16.7457089472 +49 39 02.225619216 6.17 6.700 6.748     B4V(e) 92 0

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