2000A&A...354..216B


Query : 2000A&A...354..216B

2000A&A...354..216B - Astronomy and Astrophysics, volume 354216-228 (2000/2-1)

The Pleiades, Coma, Hyades, and Praesepe open clusters: Li, Al, Si, S, Fe, Ni, and Eu abundances compared in A stars.

BURKHART C. and COUPRY M.F.

Abstract (from CDS):

In the third of a series of papers on the A stars in open clusters, the Coma and Hyades clusters are revisited; in the first and second papers, the Pleiades and Praesepe were respectively investigated. All the spectra were secured with the Canada-France-Hawaii telescope at high spectral resolution and high signal-to-noise ratios. Photospheric abundances have been determined for Li, Al, Si, S, Fe, Ni, and Eu from model atmosphere abundance analysis. All the A stars with enough-sharp lines to be studied for Li were observed in the four clusters. Abundance results are summarized for 31 cluster members, including 21 Am, 7 normal A, and 3 early-A stars. The Am stars have very uniform Li, Al, Si, S, and Fe abundances in a large temperature range of nearly 1000K. Compared to normal A stars, Li is significantly deficient in Am stars (by a factor of 3), Al marginally overabundant, Si, S, and Fe are the same, Ni and Eu (with only a few results) overabundant. Those uniform abundances of Li, Al, Si, S, or Fe in Am stars involve that abundances are little affected by the magnitude of the rotational velocity. For both Am and normal A samples, no abundance trend as a function of age and/or evolution is detected in the case of Li, Al, Si, S, or Fe. The ages considered are in the range 0.8-7x108 years; the evolution is limited from the ZAMS to the cluster turn-off. The build-up of the chemical abundances studied, in particular the Li differentiation between Am and normal A stars, could have taken place very early when the stars arrive on the Main Sequence. The spread in lithium found for the A stars is reminiscent of that reported in the field and one open cluster for stars of nearly the same mass and slightly evolved out of the Main Sequence. The Li abundance does not change as soon as the star evolves through the subgiant phase and the convection zone becomes deeper. There are two exceptional Am stars: one, in the Hyades, is Li-deficient and the other, in Praesepe, Li-overabundant. They are no obvious circumstances that can distinguish both stars from others in the very same region of their respective cluster sequence. In each of the four clusters, the maximum Li abundance is found in A stars, generally in normal A stars. The Fe abundance of both Am and normal A groups is found to be twice the original Fe value (on the ZAMS) in each of the four clusters, independently of their age or metallicity. It is well established for the Am group and in only a narrow range of Teff for the normal A group. This behavior is unexpected for normal A stars which are thought to have their original abundances and Fe abundance different from that of Am stars. A larger normal A sample is needed to conclude anything. Our abundance results for cluster Am stars quantitatively agree with predictions of new models coupling atomic diffusion with turbulent transport (Richer et al., 2000, ApJ, in press).

Abstract Copyright: ∼

Journal keyword(s): stars: abundances - stars: chemically peculiar - Galaxy: open clusters and associations: individual: Coma cluster - Galaxy: open clusters and associations: individual: Hyades - Galaxy: open clusters and associations: individual: Pleiades - Galaxy: open clusters and associations: individual: Praesepe

Simbad objects: 29

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Number of rows : 29
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 HD 22615 V* 03 39 00.0585760560 +20 54 56.784028824   6.646 6.493     A4III 66 0
2 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
3 * 60 Tau dS* 04 22 03.5181398136 +14 04 37.912925064   6.054 5.710 7.05 5.38 kA3hF2mF2(III) 288 0
4 * 63 Tau SB* 04 23 25.0640719200 +16 46 38.150834016   5.957 5.625 7.04 5.33 kA4VmF2/5IIIp 304 0
5 * del02 Tau PM* 04 24 05.7614531616 +17 26 38.871301956 5.07 4.95 4.80 4.64 4.57 A2Vs 261 0
6 * del03 Tau a2* 04 25 29.3847186643 +17 55 40.463442784   4.369 4.298 6.18 4.24 A2IV-Vs 429 0
7 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
8 HD 30210 PM* 04 46 01.7404096416 +11 42 20.112329592   5.566 5.346     Am 175 0
9 * h Ori SB* 05 09 19.6432730712 +09 49 46.502673924 5.83 5.67 5.43 5.25 5.13 A2m 263 0
10 HD 33204 SB* 05 09 45.0937327344 +28 01 49.686514248   6.296 5.997   5.69 A7VAm: 169 0
11 * mu. Ori SB* 06 02 22.99668 +09 38 50.1820 4.40     3.94 3.86 A1Vm+F2V 268 0
12 HD 73045 SB* 08 36 48.0046481184 +18 52 58.090934424   8.89 8.62     kA1hA5mA9Si 92 0
13 NGC 2632 OpC 08 39 58.4 +19 36 33           ~ 1733 0
14 HD 73709 SB* 08 40 20.7479143752 +19 41 12.242993316   7.87 7.68     kA2hA5mF0(III-IV)(Cr) 120 0
15 Cl Melotte 111 OpC 12 11 54.9 +25 16 36           ~ 520 0
16 HD 106999 ** 12 18 11.2046430672 +27 18 02.131352064   7.64 7.47     kA5hA5mF0 59 0
17 * 8 Com * 12 19 19.1929880208 +23 02 04.821806040   6.416 6.220     kA7hF2mF3 147 0
18 V* KU Com dS* 12 21 26.7390932544 +24 59 49.298164296   7.64 7.38     Am 130 0
19 HD 107655 Em* 12 22 10.8268845600 +24 46 25.918451724   6.170 6.162     A2IV 98 0
20 * 13 Com a2* 12 24 18.5489029728 +26 05 54.921403788   5.26 5.18     A3V 148 0
21 HD 108486 EB* 12 27 38.3636590224 +25 54 43.580490048   6.835 6.654     A1IV-VSrSi 138 0
22 HD 108642 SB* 12 28 38.1501425400 +26 13 37.021090692   6.71 6.54     A1IV-VSrSi 154 0
23 HD 108651 SB* 12 28 44.5650287472 +25 53 57.557921208   6.82 6.61     kA2hA9VmF0 174 0
24 * 17 Com a2* 12 28 54.7022406648 +25 54 46.265813136   5.208 5.236     B9VCrEu 288 0
25 * 21 Com a2* 12 31 00.5605002264 +24 34 01.797245328   5.496 5.436     A2pv 295 0
26 * 22 Com * 12 33 34.2193153104 +24 16 58.739975472   6.363 6.243     A4Vm 164 0
27 * gam Cap a2* 21 40 05.4454210419 -16 39 44.536313677 4.19 3.98 3.67 3.47 3.34 kF0hF1VmF2 200 0
28 HD 206546 SB* 21 43 13.5333108960 -19 37 15.462516000   6.468 6.209     A0mA5-F0 89 0
29 NGC 7789 OpC 23 57 19.4 +56 43 28   7.68 6.7     ~ 575 0

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