1998A&AS..129..237F


Query : 1998A&AS..129..237F

1998A&AS..129..237F - Astron. Astrophys., Suppl. Ser., 129, 237-266 (1998/April-2)

Abundances in metal-rich stars. Detailed abundance analysis of 47 G and K dwarf stars with [Me/H] > 0.10 dex.

FELTZING S. and GUSTAFSSON B.

Abstract (from CDS):

We have derived elemental abundances of O, Na, Mg, Al, Si, Ca, Ti, Cr, Mn, Fe, Co, Ni as well as for a number of s-elements for 47 G and K dwarf, with [Me/H]>0.1dex. The selection of stars was based on their kinematics as well as on their uvby-β photometry. One sample of stars on rather eccentric orbits traces the chemical evolution interior to the solar orbit and another, on circular orbits, the evolution around the solar orbit. A few Extreme Population I stars were included in the latter sample. The stars have -0.1dex<[Fe/H]<0.42dex. The spectroscopic [Fe/H] correlate well with the [Me/H] derived from uvby-β photometry. We find that the elemental abundances of Mg, Al, Si, Ca, Ti, Cr and Ni all follow [Fe/H]. Our data put further constraints on models of galactic chemical evolution, in particular of Cr, Mn and Co which have not previously been studied for dwarf stars with [Me/H]>0.1 dex. The increase in [Na/Fe] and [Al/Fe] as a function of [Fe/H] found previously by Edvardsson et al. (1993a) has been confirmed for [Na/Fe]. This upturning relation, and the scatter around it, are shown not to be due to a mixture of populations with different mean distances to the galactic centre. We do not confirm the same trend for aluminium, which is somewhat surprising since both these elements are thought to be produced in the same environments in the pre-supernova stars. Nor have we been able to trace any tendency for relative abundances of O, Si, and Ti relative to Fe to vary with the stellar velocities, i.e. the stars present mean distance to the galactic centre. These results imply that there is no significant difference in the chemical evolution of the different stellar populations for stars with [Me/H]>0.1dex. We find that [O/Fe] continue to decline with increasing [Fe/H] and that oxygen and europium correlate well. However [Si/Fe] and [Ca/Fe] seem to stay constant. A real ("cosmic") scatter in [Ti/Fe] at given [Fe/H] is suggested as well as a decreasing abundance of the s-elements relative to iron for the most metal-rich dwarf stars. We discuss our results in the context of recent models of galactic chemical evolution. In our sample we have included a few very metal rich stars, sometimes called SMR (super metal rich) stars. We find these stars to be among the most iron-rich in our sample but far from as metal-rich as indicated by their photometric metallicities. SMR stars on highly eccentric orbits, alleged to trace the evolution of the chemical evolution in the galactic Bulge, have previously been found overabundant in O, Mg and Si. We have included three such stars from the study by Barbuy & Grenon (1990). We find them to be less metal rich and the other elemental abundances remain puzzling. Detailed spectroscopic abundance analyses of K dwarf stars are rare. Our study includes 5 K dwarf stars and has revealed what appears to be a striking example of overionization. The overionization is especially prominent for Ca, Cr and Fe. The origin of this apparent overionization is not clear and we discuss different explanations in some detail.

Abstract Copyright:

Journal keyword(s): Galaxy: abundances - evolution - stars: abundances - late-type - fundamental parameters

VizieR on-line data: <Available at CDS (J/A+AS/129/237): table11.dat stars.dat>

Simbad objects: 47

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Number of rows : 47
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 HD 30562 PM* 04 48 36.3850851388 -05 40 26.557737782   6.40 5.77     G2IV 259 1
2 HD 32147 PM* 05 00 48.9993452248 -05 45 13.224327192 8.27 7.27 6.21 5.36 4.87 K3+V 461 1
3 HD 37088 PM* 05 36 27.4307103792 +14 39 14.868893448   9.19 8.53     G0 21 0
4 HD 36130 PM* 05 37 33.4790782824 +74 41 19.553400888       7.4   G0 65 0
5 HD 37216 PM* 05 39 52.3476047976 +52 53 50.951967360   8.60 7.83     G5V 74 0
6 HD 37986 PM* 05 41 53.6865095232 -15 37 49.950691068   8.16 7.37     G8+VCN+1 105 0
7 HD 49178 PM* 06 48 53.8179652461 +37 30 18.436463504   8.76 8.07     G0 52 0
8 HD 54322 ** 07 09 13.4937348432 +19 02 33.519724908   9.04 8.41 8.2   G5 52 0
9 HD 55693 PM* 07 13 02.6731051176 -24 13 32.068394832   7.83 7.16     G1.5V 93 0
10 HD 61606 BY* 07 39 59.3286138624 -03 35 51.027583488 8.89 8.136 7.169 6.626 6.15 K3V 195 0
11 * mu.02 Cnc PM* 08 07 45.8562513552 +21 34 54.526814256 6.14 5.93 5.30     G1IVb 226 0
12 HD 69582 SB* 08 17 29.6055783480 -03 06 27.227814300   8.28 7.56     G5/6V 23 0
13 HD 68988 PM* 08 18 22.1728652088 +61 27 38.595044628   8.84 8.19     G1V 155 2
14 HD 69830 PM* 08 18 23.9469682407 -12 37 55.817187530   6.74 5.95     G8:V 526 1
15 HD 71479 PM* 08 27 35.1263140176 -05 08 55.091299884   7.81 7.18     G2/3V 92 0
16 HD 72946 PM* 08 35 51.2666658240 +06 37 21.954760284 8.23     6.7   G8-V 124 0
17 HD 75782 PM* 08 53 11.5182806712 +37 04 13.000010016       6.7   G0 57 0
18 HD 76780 PM* 08 58 55.7308254024 +21 09 58.637729628   8.32 7.63     G5 62 0
19 HD 77338 PM* 09 01 12.4934924904 -25 31 37.432543296   9.47 8.59     K0IV 70 1
20 HD 80607 PM* 09 22 39.7366541424 +50 36 13.952919312   9.937 9.070     G5 100 2
21 HD 87007 PM* 10 01 58.5834562296 -10 24 19.411744716   9.60 8.73     K0V 38 0
22 HD 87646 ** 10 06 40.7699030736 +17 53 42.278595144   8.73 8.07     G2V 66 0
23 HD 91204 * 10 32 05.5005044280 +17 59 23.044554276   8.44 7.82     G0 62 0
24 HD 94835 PM* 10 57 09.5535647640 +21 48 17.544606048   8.59   7.5   G0 73 0
25 HD 101242 PM* 11 39 01.0011622267 +06 03 28.450096767   8.30   7.2   G5 62 0
26 HD 103932 PM* 11 57 56.2063477236 -27 42 25.366588848 9.23 8.114 6.964 6.298 5.758 K4+V 160 0
27 HD 106156 PM* 12 12 57.5317999258 +10 02 15.776359716   8.71   7.4   G8V 96 0
28 HD 110010 SB* 12 37 19.3007880240 +79 12 56.040453936 7.830 7.610 6.990     G0 79 0
29 HD 117243 PM* 13 28 39.2923760184 +28 26 54.924465948       7.9   G5III 43 0
30 HD 125968 PM* 14 23 23.3801291980 -27 49 21.670846371   8.42 7.76     G3/5V 55 0
31 HD 126511 PM* 14 24 48.9417591696 +41 16 30.390340080       7.9   G5 53 0
32 V* KU Lib BY* 14 40 31.1063299272 -16 12 33.452598312 8.247 7.977 7.240 6.837 6.47 G8Vk: 98 0
33 HD 130087 PM* 14 45 56.7854632224 +10 03 07.225257564   8.13 7.51     G2IV 64 0
34 HD 131977 BY* 14 57 28.0007918772 -21 24 55.727265310 7.89 6.83 5.72 4.74 4.19 K4V 485 0
35 HD 134474 PM* 15 08 58.7402246376 +37 19 06.810625200   9.69 8.84     G5 36 0
36 * 23 Lib PM* 15 13 28.6669233518 -25 18 33.653388418   7.168 6.46 6.43   G6IV-V 303 1
37 HD 136834 PM* 15 22 42.5465323962 +01 25 07.052636328   9.30   8.738   K3IV-V 139 0
38 HD 137510 PM* 15 25 53.2697518752 +19 28 50.545457724   6.872 6.241     G0IV-V 110 0
39 HD 144585 PM* 16 07 03.3696573456 -14 04 16.671141984 7.22 6.98 6.32     G2V 191 0
40 HD 171999 SB* 18 37 58.8187971885 -06 48 19.714925000   9.18 8.30 7.8   K0IV/V 81 1
41 HD 175518 SB* 18 55 52.9705387088 -05 44 42.797045543   8.21 7.46     G6IV/V 77 0
42 HD 178911 SB* 19 09 04.3519341413 +34 36 01.242009328   7.37   6.3   G1V+K1V 135 0
43 HD 180890 PM* 19 17 37.7317012296 +19 09 39.311453916   9.09 8.32     G5 19 0
44 * b Aql PM* 19 24 58.1999714302 +11 56 39.888480530 6.35 5.93   4.7   G7IVHdel1 490 0
45 HD 183263 * 19 28 24.5713671072 +08 21 29.004515424   8.51 7.86     G6IV 129 1
46 * 16 Cyg B PM* 19 41 51.9726777456 +50 31 03.089030916 7.07 6.86 6.20 5.76 5.42 G3V 890 1
47 HD 187055 PM* 19 45 30.3415420174 +50 46 21.845092718       8.4   G9V 42 0

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