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| 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):
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
| 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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