2002MNRAS.333..121S


Query : 2002MNRAS.333..121S

2002MNRAS.333..121S - Mon. Not. R. Astron. Soc., 333, 121-132 (2002/June-2)

Merged binary white dwarf evolution: rapidly accreting carbon-oxygen white dwarfs and the progeny of extreme helium stars.

SAIO H. and JEFFERY C.S.

Abstract (from CDS):

We have examined the evolution of merged low-mass double white dwarfs that become luminous helium stars. We have approximated the merging process by the rapid accretion of matter, consisting mostly of helium, on to a carbon-oxygen (CO) white dwarf. After a certain mass is accumulated, a helium shell flash occurs, the radius and luminosity increase and the star becomes a yellow giant. Mass accretion is stopped artificially when the total mass reaches a pre-determined value. When the mass above the helium-burning shell becomes small enough, the star evolves blueward almost horizontally in the Hertzsprung-Russell diagram. The theoretical models for the merger of a 0.6-M☉ CO white dwarf with a 0.3-M☉ He white dwarf agree very well with the observed locations of extreme helium stars in the logTeff-logg diagram, with their observed rates of blueward evolution, and with luminosities and masses obtained from their pulsations. Together with predicted merger rates for CO+He white dwarf pairs, the evolutionary time-scales are roughly consistent with the observed numbers of extreme helium stars. Predicted surface carbon and oxygen abundances can be consistent with the observed values if carbon and oxygen produced in the helium shell during a previous asymptotic giant branch phase are assumed to exist in the helium zone of the initial CO white dwarfs. These results establish the CO+He white dwarf merger as the best, if not only, viable model for the creation of extreme helium stars and, by association, the majority of R Coronae Borealis stars.

Abstract Copyright: 2002 Blackwell Science Ltd

Journal keyword(s): binaries: close - stars: chemically peculiar - stars: evolution - white dwarfs

Simbad objects: 22

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Number of rows : 22
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 2MASS J06544616-1048325 pA* 06 54 46.1643701544 -10 48 32.601721752   12.99 12.27 12.08   OB+ 23 0
2 V* DN Leo Pu* 10 38 55.2343433712 +10 03 48.486337812   9.76 9.93     Bp 150 0
3 V* DY Cen RC* 13 25 34.0847063328 -54 14 43.129581792     12.00     C-Hd/B5-6Ie 105 0
4 V* BX Cir Pu* 14 01 36.4829811264 -66 09 56.163698820 11.79 12.62 12.58 12.75   OB+ 69 0
5 V* V821 Cen Pu* 14 14 58.6292612424 -46 17 19.294106424 9.09 9.89 9.98     (B)p 145 0
6 HD 144941 pA* 16 09 24.5513020968 -27 13 38.184011148 9.45 10.17 10.02     B8 96 1
7 V* V2205 Oph Pu* 16 28 35.3724415104 -09 19 31.849139568 9.79 10.56 10.5     B 102 0
8 V* V652 Her pA* 16 48 04.6934854032 +13 15 42.420402252   10.31 10.51     ~ 147 0
9 HD 160641 HS* 17 41 51.5791786632 -17 53 48.462200880 9.15 10.01 9.85 10.08 9.59 sdOC9.5II-IIIHe40 128 0
10 CD-46 11775 pA* 17 42 33.9915492936 -46 58 48.829063584   11.14 11.27     OB+ 43 0
11 2MASS J17442550-1937537 pA* 17 44 25.5054075744 -19 37 53.754611844   12.8 12.60 12.62   OB+ 25 0
12 LS IV -01 2 Pu* 17 51 26.8365068760 -01 43 21.127711008 10.88 11.4 10.9     OB+ 52 0
13 V* V4334 Sgr CV* 17 52 32.69352 -17 41 08.0160           F2Ia 390 0
14 V* NO Ser Pu* 18 03 55.5266289144 -01 00 23.228086608 10.53 10.7 10.3     B 65 0
15 LS IV +06 2 HS* 18 06 55.4522031744 +06 21 57.246453756   12.11 12.14 12.32   sdBC1VHe39 37 0
16 V* PV Tel s?b 18 23 14.6623123440 -56 37 44.138664012 8.60 9.20 9.30     B5?I?pec 130 0
17 V* MV Sgr RC* 18 44 31.9665722184 -20 57 12.863610864 12.82 13.56 12.00 13.37   B2pec-Hd 111 0
18 V* V4732 Sgr Pu* 18 59 39.5771671848 -14 26 17.543500548 11.19 11.5 10.9     OB+ 42 0
19 PN A66 58 PN 19 18 20.476 +01 46 59.62           [WC4] 327 0
20 V* V1920 Cyg Pu* 19 45 17.2712347176 +33 58 26.596281540 9.81 10.41 10.18   10.134 B2/3 52 0
21 Hen 1-5 pA* 20 11 56.0595568008 +20 20 04.420944132 11.41 10.66 9.45     G8/K0Iae 523 0
22 V* FQ Aqr Pu* 20 51 21.3360113136 +02 18 46.360439064 9.18 9.62 9.52     F 71 0

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