2015A&A...577A..55D


Query : 2015A&A...577A..55D

2015A&A...577A..55D - Astronomy and Astrophysics, volume 577A, 55-55 (2015/5-1)

Non-conservative evolution in Algols: where is the matter?

DESCHAMPS R., BRAUN K., JORISSEN A., SIESS L., BAES M. and CAMPS P.

Abstract (from CDS):

There is indirect evidence of non-conservative evolutions in Algols. However, the systemic mass-loss rate is poorly constrained by observations and generally set as a free parameter in binary-star evolution simulations. Moreover, systemic mass loss may lead to observational signatures that still need to be found. Within the ''hotspot'' ejection mechanism, some of the material that is initially transferred from the companion star via an accretion stream is expelled from the system due to the radiative energy released on the gainer's surface by the impacting material. The objective of this paper is to retrieve observable quantities from this process and to compare them with observations. We investigate the impact of the outflowing gas and the possible presence of dust grains on the spectral energy distribution (SED). We used the 1D plasma code Cloudy and compared the results with the 3D Monte-Carlo radiative transfer code Skirt for dusty simulations. The circumbinary mass-distribution and binary parameters were computed with state-of-the-art binary calculations done with the Binstar evolution code.The outflowing material reduces the continuum flux level of the stellar SED in the optical and UV. Because of the time-dependence of this effect, it may help to distinguish between different ejection mechanisms. If present, dust leads to observable infrared excesses, even with low dust-to-gas ratios, and traces the cold material at large distances from the star. By searching for this dust emission in the WISE catalogue, we found a small number of Algols showing infrared excesses, among which the two rather surprising objects SX Aur and CZ Vel. We find that some binary B[e] stars show the same strong Balmer continuum as we predict with our models. However, direct evidence of systemic mass loss is probably not observable in genuine Algols, since these systems no longer eject mass through the hotspot mechanism. Furthermore, owing to its high velocity, the outflowing material dissipates in a few hundred years. If hot enough, the hotspot may produce highly ionised species, such as SiIV, and observable characteristics that are typical of W Ser systems. If present, systemic mass loss leads to clear observational imprints. These signatures are not to be found in genuine Algols but in the closely related β Lyraes, W Serpentis stars, double periodic variables, symbiotic Algols, and binary B[e] stars. We emphasise the need for further observations of such objects where systemic mass loss is most likely to occur.

Abstract Copyright:

Journal keyword(s): binaries: general - radiative transfer - circumstellar matter - methods: numerical

Simbad objects: 34

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Number of rows : 34
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11145 1
2 * phi Per Be* 01 43 39.6379691568 +50 41 19.433124998 3.10 4.02 4.06 3.90 3.88 B1.5V:e-shell 571 0
3 V* RX Cas EB* 03 07 45.7479808272 +67 34 38.612093520   10.14 8.64     K1III+A5eIII 183 0
4 * bet Per EB* 03 08 10.1324535 +40 57 20.328013 1.70 2.07 2.12 2.08 2.11 B8V 1219 1
5 V* AS Eri EB* 03 32 25.1263057224 -03 18 48.095135748   8.49 8.30     A3V+K0III 172 0
6 HD 33357 Be* 05 11 42.9274371912 +42 09 55.275165324 7.67 8.55 8.55     B1:V:ne 181 0
7 HD 37453 * 05 39 56.6240145063 +30 05 11.239856996   8.90 8.16     F4III 42 0
8 HD 41335 Be* 06 04 13.5003372120 -06 42 32.225392980 4.31 5.14 5.21 5.13 5.09 B1V 299 0
9 * 17 Lep Sy* 06 04 59.1294521328 -16 29 03.969238632 5.29 5.17 4.93     A3+K/M 210 0
10 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 742 2
11 HD 43246 SB* 06 16 22.1977904160 +28 51 07.127565372   7.82 7.41     A0Vn+F5III 49 0
12 HD 45910 Be* 06 30 32.9373877056 +05 52 01.204796244 6.64 7.18 6.85 6.31 5.81 B2IIIe 227 0
13 V* V509 Mon EB* 06 47 10.7214399312 -01 02 14.736207228     14.42     G4IV 10 0
14 HD 50846 EB* 06 54 54.7081653504 -01 22 32.850081768   8.46 8.43     B5/7Ib 149 0
15 HD 51480 Be* 06 57 09.3836145600 -10 49 28.065280368 6.66 7.24 6.93 7.78   B3/5Ibe 93 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* DM Pup EB* 08 07 04.0941308064 -25 31 52.242779892           A2.5 6 0
18 V* CZ Vel EB* 09 10 44.4645889080 -50 42 40.609091376   11.57 10.80     B6 12 0
19 V* W Cru EB* 12 11 59.1619876512 -58 47 00.736976220   9.47 8.44     F8/G1Ia/abe 99 0
20 V* U CrB EB* 15 18 11.3524167096 +31 38 49.412401368   7.79 7.83     B6V 260 0
21 V* UZ Nor EB* 16 28 11.5597611312 -53 19 21.648325728 11.09 11.34 11.29     B 11 0
22 V* W Ser EB* 18 09 50.6485613712 -15 33 00.263398644   9.64 8.42     F8/G2Iaep(+A) 136 0
23 V* RY Sct Be* 18 25 31.4771300232 -12 41 24.192361500 10.25 10.38 9.12 9.46   O9.7Ibep 300 2
24 V* RZ Sct EB* 18 26 33.5232714792 -09 12 05.987275200 8.09 8.24 7.53     B2/3Ib/II 170 0
25 V* V930 Oph EB* 18 41 45.6494492208 +12 02 11.116220928     12.97     ~ 8 0
26 HD 174237 Be* 18 46 43.0891606728 +52 59 16.654686648 5.06 5.80 5.90     B3+F5III 203 0
27 V* DH Her EB* 18 47 34.5584574552 +22 50 45.797192304   10.55 10.50     A5 26 0
28 V* V356 Sgr EB* 18 47 52.3312296264 -20 16 28.243688340   7.07 6.99     B9III 173 0
29 * 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
30 HD 198288 EB* 20 47 59.5845423048 +39 17 15.717392988 8.080 7.72 7.06     A3Ibep 205 0
31 HD 207739 SB* 21 49 58.8414553632 +43 57 56.833528572   9.22 8.59     kF0:mGepec 64 0
32 * pi. Aqr Be* 22 25 16.6230017410 +01 22 38.634449478 3.64 4.60 4.64 4.48 4.48 B1III-IVe 415 0
33 HD 218393 Be* 23 07 06.2121558408 +50 11 32.488582812 6.79 7.25 6.92     B3pe+K1III 154 0
34 V* V442 Cas EB* 23 40 14.7999477864 +53 57 33.991392600   13.06 12.74     M5V 19 0

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