2015A&A...573A.107H


Query : 2015A&A...573A.107H

2015A&A...573A.107H - Astronomy and Astrophysics, volume 573A, 107-107 (2015/1-1)

Properties and nature of Be stars. 30. Reliable physical properties of a semi-detached B9.5e+G8III binary BR CMi = HD 61273 compared to those of other well studied semi-detached emission-line binaries.

HARMANEC P., KOUBSKY P., NEMRAVOVA J.A., ROYER F., BRIOT D., NORTH P., LAMPENS P., FREMAT Y., YANG S., BOZIC H., KOTKOVA L., SKODA P., SLECHTA M., KORCAKOVA D., WOLF M. and ZASCHE P.

Abstract (from CDS):

Reliable determination of the basic physical properties of hot emission-line binaries with Roche-lobe filling secondaries is important for developing the theory of mass exchange in binaries. It is a very hard task, however, which is complicated by the presence of circumstellar matter in these systems. So far, only a small number of systems with accurate values of component masses, radii, and other properties are known. Here, we report the first detailed study of a new representative of this class of binaries, BR CMi, based on the analysis of radial velocities and multichannel photometry from several observatories, and compare its physical properties with those for other well-studied systems. BR CMi is an ellipsoidal variable seen under an intermediate orbital inclination of ∼51°, and it has an orbital period of 12.919059(15)d and a circular orbit. We used the disentangled component spectra to estimate the effective temperatures 9500(200) K and 4655(50) K by comparing them with model spectra. They correspond to spectral types B9.5e and G8III. We also used the disentangled spectra of both binary components as templates for the 2D cross-correlation to obtain accurate radial velocities and a reliable orbital solution. Some evidence of a secular period increase at a rate of (1.1±0.5) s per year was found. This, together with a very low mass ratio of 0.06 and a normal mass and radius of the mass gaining component, indicates that BR CMi is in a slow phase of the mass exchange after the mass-ratio reversal. It thus belongs to a still poorly populated subgroup of Be stars for which the origin of Balmer emission lines is safely explained as a consequence of mass transfer between the binary components.

Abstract Copyright:

Journal keyword(s): binaries: close - binaries: spectroscopic - stars: emission-line, Be - stars: individual: BR CMi (HD 61273) - stars: fundamental parameters

Simbad objects: 27

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Number of rows : 27
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 232121 EB* 00 10 42.0679172568 +54 53 29.361482988   9.67 8.97     B5+K3III 182 0
2 V* RX Cas EB* 03 07 45.7479808272 +67 34 38.612093520   10.14 8.64     K1III+A5eIII 183 0
3 HD 37453 * 05 39 56.6240145063 +30 05 11.239856996   8.90 8.16     F4III 42 0
4 HD 43246 SB* 06 16 22.1977904160 +28 51 07.127565372   7.82 7.41     A0Vn+F5III 49 0
5 V* HZ CMa Be* 06 50 23.3482557912 -31 42 21.808309320   5.829 5.747     B6IVe+A 91 0
6 HD 50846 EB* 06 54 54.7081653504 -01 22 32.850081768   8.46 8.43     B5/7Ib 149 0
7 HD 51956 SB* 06 59 31.7494168896 +00 55 00.357446136   8.31 7.51     F6Ib/II 41 0
8 * 1 CMi * 07 24 58.1800202736 +11 40 10.282487304   5.461 5.361     A5IV 46 0
9 HD 59059 * 07 28 47.2558472952 +15 06 35.365121100 6.06 6.17 6.22     B9IV 44 0
10 HD 59771 Em* 07 30 51.0694348656 -18 15 42.499944828   9.80 8.96     F2/3II 18 0
11 V* BR CMi a2* 07 38 50.9832531024 +07 57 59.643300708   7.36 7.15     B9.5+G8III 30 0
12 BD+08 1835 * 07 39 08.4550660776 +08 00 23.174955396   9.76 9.60     A2 2 0
13 HD 61341 * 07 39 09.6966497640 +07 49 51.442571964   8.16 7.96     A2 14 0
14 * bet Gem PM* 07 45 18.94987 +28 01 34.3160 3.00 2.14 1.14 0.39 -0.11 K0IIIb 1101 2
15 V* PW Pup EB* 07 49 06.0103241448 -31 07 42.625060284 10.54 10.23 9.53 9.85   G0Ie 39 0
16 V* UX Mon EB* 07 59 16.3752271920 -07 30 17.892250632   8.74 8.42     A2/3+G/K 129 0
17 V* TT Hya EB* 11 13 12.4976326464 -26 27 54.253972800   7.43 7.31     F0IV:kA2mA3:_sh 188 0
18 V* BY Cru EB* 12 04 48.6318279024 -62 00 08.193672324 7.85 8.18 7.63 8.70   F0Ib/II 38 0
19 HD 127208 Be* 14 30 40.4651520192 -22 27 39.310443504   7.12 6.96     B9IVe 40 0
20 * del Sco SB* 16 00 20.00528 -22 37 18.1431 1.30 2.20 2.32 2.36 2.49 B0.3IV 740 0
21 V* V393 Sco EB* 17 48 47.6035402728 -35 03 25.629637680   7.71 7.59     B3III 68 0
22 HD 174237 Be* 18 46 43.0891606728 +52 59 16.654686648 5.06 5.80 5.90     B3+F5III 203 0
23 * bet Lyr EB* 18 50 04.7951442356 +33 21 45.600371200 2.85 3.42 3.42 3.31 3.29 B8.5Ib-II 926 0
24 V* V448 Cyg SB* 20 06 09.9484340064 +35 23 09.618394920 7.89 8.45 8.16     O9.5V+B1Ib 152 0
25 HD 207739 SB* 21 49 58.8414553632 +43 57 56.833528572   9.22 8.59     kF0:mGepec 64 0
26 * 14 Lac EB* 22 50 21.7785565224 +41 57 12.221400240 5.49 5.961 5.910     B4+F9III 149 0
27 HD 218393 Be* 23 07 06.2121558408 +50 11 32.488582812 6.79 7.25 6.92     B3pe+K1III 154 0

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