2001MNRAS.324..937P


Query : 2001MNRAS.324..937P

2001MNRAS.324..937P - Mon. Not. R. Astron. Soc., 324, 937-959 (2001/July-2)

Abundance analyses of cool extreme helium stars.

PANDEY G., RAO N.K., LAMBERT D.L., JEFFERY C.S. and ASPLUND M.

Abstract (from CDS):

Extreme helium stars (EHes) with effective temperatures from 8000 to 13000K are among the coolest EHes and overlap the hotter R CrB stars in effective temperature. The cool EHes may represent an evolutionary link between the hot EHes and the R CrB stars. Abundance analyses of four cool EHes, BD+1°4381 (FQ Aqr), LS IV -14°109, BD -1°3438 (NO Ser) and LS IV -1°002 (V2244 Oph), are presented. All these stars show evidence of H- and He-burning at earlier stages of their evolution.

To test for an evolutionary connection, the chemical compositions of cool EHes are compared with those of hot EHes and R CrB stars. Relative to Fe, the N abundance of these stars is intermediate between those of hot EHes and R CrB stars. For the R CrB stars, the metallicity M derived from the mean of Si and S appears to be more consistent with the kinematics than that derived from Fe. When metallicity M derived from Si and S replaces Fe, the observed N abundances of EHes and R CrB stars fall at or below the upper limit corresponding to thorough conversion of initial C and O to N. There is an apparent difference between the composition of R CrB stars and EHes, the former having systematically higher [N/M] ratios. The material present in the atmospheres of many R CrB stars is heavily CN- and ON-cycled. Most of the EHes have only CN-cycled material in their atmospheres. There is an indication that the CN- and ON-cycled N in EHes was partially converted to Ne by α-captures. If EHes are to evolve to R CrB stars, fresh C in EHes has to be converted to N; the atmospheres of EHes have just sufficient hydrogen to raise the N abundance to the level of R CrB stars. If Ne is found to be normal in R CrB stars, the proposal that EHes evolve to R CrB stars fails. The idea that R CrB stars evolve to EHes is ruled out; the N abundance in R CrB stars has to be reduced to the level of EHes, as the C/He, which is observed to be uniform across EHes, has to be maintained. Hence the inferred [N/M], C/He and [Ne/M] ratios, and the H-abundances of these two groups indicate that the EHes and the R CrB stars may not be on the same evolutionary path.

The atmospheres of H-deficient stars probably consist of three ingredients: a residue of normal H-rich material, substantial amounts of H-poor CN(O)-cycled material, and C- (and O-) rich material from gas exposed to He-burning. This composition could be a result of final He-shell flash in a single post-AGB star (FF scenario), or a merger of two white dwarfs (DD scenario). Although the FF scenario accounts for Sakurai's object and other stars (e.g., the H-poor central stars of planetary nebulae), present theoretical calculations imply higher C/He and O/He ratios than are observed in EHes and R CrB stars. Quantitative predictions are lacking for the DD scenario.


Abstract Copyright: The Royal Astronomical Society

Journal keyword(s): stars: abundances - stars: AGB and post-AGB - stars: chemically peculiar - stars: evolution

Simbad objects: 40

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Number of rows : 40
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 V* XX Cam RC* 04 08 38.7489702792 +53 21 39.350441448 8.35 8.10 7.27     F8I 145 0
2 V* SU Tau RC* 05 49 03.7301227728 +19 04 21.867600252   10.72 9.10     C1,0_Hd_CH0 157 1
3 2MASS J06544616-1048325 pA* 06 54 46.1643701544 -10 48 32.601721752   12.99 12.27 12.08   OB+ 23 0
4 V* DN Leo Pu* 10 38 55.2343433712 +10 03 48.486337812   9.76 9.93     Bp 150 0
5 V* UX Ant RC* 10 57 09.0588420456 -37 23 55.133370312   12.67 12.37     C-Hd 48 0
6 V* UW Cen RC* 12 43 17.1901954368 -54 31 40.763998596   10.84 10.13     K 123 0
7 V* Y Mus RC* 13 05 48.1948797744 -65 30 46.624502484   11.3 10.50     Fp_Hd 79 0
8 V* DY Cen RC* 13 25 34.0847063328 -54 14 43.129581792     12.00     C-Hd/B5-6Ie 105 0
9 CD-46 8926 HS* 13 53 08.2139106408 -46 43 42.314548008   11.04 11.30     sdO 51 0
10 V* BX Cir Pu* 14 01 36.4829811264 -66 09 56.163698820 11.79 12.62 12.58 12.75   OB+ 69 0
11 V* V821 Cen Pu* 14 14 58.6292612424 -46 17 19.294106424 9.09 9.89 9.98     (B)p 145 0
12 V* V854 Cen RC* 14 34 49.4024471640 -39 33 19.201288284   7.13 11.69     Ce 214 0
13 V* R CrB RC* 15 48 34.4154827352 +28 09 24.295852440 6.44 6.31 5.71 5.26 5.08 G0Iep 798 0
14 HD 144941 pA* 16 09 24.5513020968 -27 13 38.184011148 9.45 10.17 10.02     B8 96 1
15 V* RT Nor RC* 16 24 18.6679360920 -59 20 38.565480480   11.34 10.60     R 85 0
16 V* V2205 Oph Pu* 16 28 35.3724415104 -09 19 31.849139568 9.79 10.56 10.5     B 102 0
17 V* RZ Nor RC* 16 32 41.66 -53 15 33.2     10.63     C-Hd 68 0
18 V* V652 Her pA* 16 48 04.6934854032 +13 15 42.420402252   10.31 10.51     ~ 147 0
19 LSE 259 HS* 16 53 54.5759529408 -56 01 54.753819672       12.707   sdO 36 1
20 CD-46 11775 pA* 17 42 33.9915492936 -46 58 48.829063584   11.14 11.27     OB+ 43 0
21 2MASS J17442550-1937537 pA* 17 44 25.5054075744 -19 37 53.754611844   12.8 12.60 12.62   OB+ 25 0
22 LS IV -01 2 Pu* 17 51 26.8365068760 -01 43 21.127711008 10.88 11.4 10.9     OB+ 52 0
23 V* NO Ser Pu* 18 03 55.5266289144 -01 00 23.228086608 10.53 10.7 10.3     B 65 0
24 LS IV +06 2 HS* 18 06 55.4522031744 +06 21 57.246453756   12.11 12.14 12.32   sdBC1VHe39 37 0
25 V* V3795 Sgr RC* 18 13 23.5642449000 -25 46 40.857266928       10.940 10.10 ~ 48 0
26 V* VZ Sgr RC* 18 15 08.5724613648 -29 42 29.491053228   11.15 10.46     ~ 57 0
27 V* RS Tel RC* 18 18 51.2223564000 -46 32 53.427456132   10.80 9.96     R0 84 1
28 V* PV Tel s?b 18 23 14.6623123440 -56 37 44.138664012 8.60 9.20 9.30     B5?I?pec 130 0
29 V* GU Sgr RC* 18 24 15.5810208792 -24 15 26.353387944   11.40 11.33     R0 70 0
30 V* MV Sgr RC* 18 44 31.9665722184 -20 57 12.863610864 12.82 13.56 12.00 13.37   B2pec-Hd 111 0
31 V* FH Sct RC* 18 45 14.8470961608 -09 25 36.106185432           C 37 0
32 V* V CrA RC* 18 47 32.3096196393 -38 09 32.307864378       10.765   R0 114 0
33 V* V4732 Sgr Pu* 18 59 39.5771671848 -14 26 17.543500548 11.19 11.5 10.9     OB+ 42 0
34 CD-51 11879 HS* 19 02 11.7428660328 -51 30 09.561616380   11.44 11.55     sdO 43 0
35 V* RY Sgr RC* 19 16 32.7668605944 -33 31 20.340212592 6.20 6.27 6.25     Cpec 370 0
36 V* V1920 Cyg Pu* 19 45 17.2712347176 +33 58 26.596281540 9.81 10.41 10.18   10.134 B2/3 52 0
37 V* V482 Cyg RC* 19 59 42.5731664472 +33 59 27.937220100   12.91 11.36   9.029 C-Hd 72 0
38 Hen 1-5 pA* 20 11 56.0595568008 +20 20 04.420944132 11.41 10.66 9.45     G8/K0Iae 523 0
39 V* FQ Aqr Pu* 20 51 21.3360113136 +02 18 46.360439064 9.18 9.62 9.52     F 71 0
40 V* UV Cas RC* 23 02 14.6592341400 +59 36 36.693038052   11.89 11.80     F0/5Ib 68 0

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