2004ApJ...613.1202B


Query : 2004ApJ...613.1202B

2004ApJ...613.1202B - Astrophys. J., 613, 1202-1212 (2004/October-1)

The correlation of lithium and beryllium in F and G field and cluster dwarf stars.

BOESGAARD A.M., ARMENGAUD E., KING J.R., DELIYANNIS C.P. and STEPHENS A.

Abstract (from CDS):

Although Li has been extensively observed in main-sequence field and cluster stars, there are relatively fewer observations of Be. We have obtained Keck HIRES spectra of 36 late F and early G dwarfs in order to study the Li-Be correlation we found previously in the temperature regime of 5900-6650 K. The sample size for this temperature range with detectable and (usually) depleted Li and Be is now 88, including Li and Be abundances in both cluster and field stars. Therefore we can now investigate the influence of other parameters such as age, temperature, and metallicity on the correlation. The Be spectra at 3130 Å were taken over six nights from 1999 November to 2002 January and have a spectral resolution of ∼48,000 and a median signal-to-noise ratio (S/N) of 108/pixel. We obtained Li spectra of 22 stars with the University of Hawaii 88 inch (2.2 m) telescope and coudé spectrograph with a spectral resolution of ∼70,000 and a median S/N of 110/pixel. We have redetermined the effective temperatures for all the stars and adopted other parameters from published data or empirical relations. The abundances of both Li and Be in the stars we observed were determined from spectrum synthesis with MOOG 2002. The previously observed Li equivalent widths for some of our Be stars were used with the new temperatures and MOOG 2002 in the ``blends'' mode. For the 46 field stars from this and earlier studies we find a linear relation between A(Li) and A(Be) with a slope of 0.375±0.036. Over the Teffrange 5900-6650 K, we find the modest scatter about the Be-Li relation to be significantly correlated with Teffand perhaps also [Fe/H]. Dividing the sample into two temperature regimes of 6300-6650 K (corresponding to the cool side of the Li-Be dip) and 5900-6300 K (corresponding to the Li ``plateau'') reveals possible small differences in the slopes for the two groups, 0.404±0.034 and 0.365±0.049, respectively. When we include the cluster stars (Hyades, Pleiades, Praesepe, UMa Group, and Coma), the slope for the full temperature range (88 stars) is essentially the same, at 0.382±0.030, as for the field stars alone. For the hotter temperature group of 35 Li-Be dip stars in the field and in clusters the slope is higher, at 0.433±0.036, while for the cooler star group (54 stars) the slope is 0.337±0.031, different by more than 1 σ. This small difference in the slope is predicted by the theory of rotationally induced mixing. The four stars with [Fe/H] less than -0.4 are all below the best-fit relation, i.e., there is more Be depletion at a given A(Li) or less Be ab initio. The youngest stars, i.e., Pleiades, have less depletion of both Li and Be. This too is predicted by rotationally induced slow mixing. Combining the Be results from both field and cluster stars, we find that there are stars with undepleted Be, i.e., near the meteoritic values of 1.42 dex, at all temperatures from 5500 to 6800 K. Depletions of Be of up to and even exceeding 2 orders of magnitude are common between 6000 and 6700 K.

Abstract Copyright:

Journal keyword(s): Stars: Abundances - Stars: Evolution

Simbad objects: 50

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Number of rows : 50
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 * 6 Cet PM* 00 11 15.8580395472 -15 28 04.720468404 5.35 5.38 4.89     F8VFe-0.8CH-0.5 312 0
2 HD 2454 SB* 00 28 20.0424818616 +10 11 23.297664120   6.47   5.8   F5VSr 177 0
3 * 61 Psc PM* 00 47 54.8276045136 +20 55 31.242238356   7.04   6.2   F8V 52 0
4 * 77 Psc A PM* 01 05 49.2273145104 +04 54 30.156785496           F5V 95 0
5 * 77 Psc B ** 01 05 51.4332128088 +04 54 33.781552200           F5/7(V) 96 0
6 * 44 And PM* 01 10 18.7404097416 +42 04 53.309986932   6.249 5.665     F8V 183 0
7 * 37 Cet ** 01 14 24.0406960100 -07 55 22.172965574   5.59 5.13     F5V 199 1
8 * 38 Cet PM* 01 14 49.1725004760 -00 58 25.659970248   6.12 5.69     F3V 115 0
9 HD 8671 PM* 01 26 18.6862929120 +43 27 27.869935680   6.464 5.978     F7V 77 0
10 * ups And PM* 01 36 47.8415443907 +41 24 19.651368029 4.70 4.64 4.10 3.64 3.35 F9V 963 1
11 HD 11592 PM* 01 53 57.6820221059 +10 36 50.490634992   7.24   6.5   F6 87 0
12 * 13 Tri PM* 02 28 48.4944856357 +29 55 54.328558216   6.478 5.901     G0V 156 0
13 * rho Ari PM* 02 56 26.1717266513 +18 01 23.665188613   6.02 5.58 5.3   F6V 158 0
14 HD 20853 * 03 20 45.2036281632 -26 36 23.428639260   6.943 6.404     F7V 35 0
15 Cl Melotte 20 OpC 03 26 28.1 +48 58 30           ~ 861 0
16 * 10 Tau PM* 03 36 52.3837044168 +00 24 05.992097829 5.23 5.15 4.30 4.09 3.77 F9IV-V 565 0
17 Cl Melotte 22 OpC 03 46 24.2 +24 06 50           ~ 3435 0
18 Cl Melotte 25 OpC 04 29 47.3 +16 56 53           ~ 3074 0
19 HD 57517 PM* 07 21 16.8135695856 -08 52 40.081627668   7.080 6.553     G1V 60 0
20 HD 58551 PM* 07 26 50.2570417275 +21 32 08.355498800   7.00   6.3   F6V 134 0
21 HD 59380 SB* 07 29 25.6609863875 -07 33 04.450065996   6.327 5.853     F6V 95 0
22 HD 70110 PM* 08 20 12.9995585712 -00 54 33.529605120   6.763 6.177     G0V 122 0
23 HD 72945 SB* 08 35 50.9775809112 +06 37 12.769503348 6.55     5.6   F8V 123 0
24 NGC 2632 OpC 08 40 13.0 +19 37 16           ~ 1564 0
25 HD 78366 PM* 09 08 51.0703818408 +33 52 55.986351384   6.53   5.6   G0IV-V 247 0
26 HD 103799 PM* 11 57 14.5832839344 +40 20 37.463173692       6.3   F6V 74 0
27 NAME Ursa Major Moving Group MGr 12 32 +57.0           ~ 439 2
28 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 4803 2
29 NAME Ursa Major Cluster ClG 15 08.8 +67 07           ~ 410 0
30 * b Her SB* 18 07 01.5906608928 +30 33 43.584892488 5.52 5.67 5.13 4.61 4.28 F6V 465 0
31 * 110 Her PM* 18 45 39.7256792847 +20 32 46.713086264 4.66 4.65 4.19 3.80 3.54 F5.5IV-V 407 0
32 * 3 Cyg ** 19 25 25.7579593032 +24 54 45.990132161   6.70   5.9   F8 97 0
33 HD 186226 PM* 19 42 45.8754597888 +08 22 57.945020304   7.35 6.83     F5 41 0
34 HD 186379 PM* 19 43 07.0299027408 +24 35 52.587634884   7.41   6.5   F8V 88 0
35 * 15 Del PM* 20 49 37.7673041328 +12 32 42.458877780   6.421 5.991     F5V 92 0
36 HD 199260 PM* 20 56 47.3316655128 -26 17 46.960329480   6.20 5.70     F6V 115 0
37 * 11 Aqr PM* 21 00 33.8408325744 -04 43 48.934668864   6.819 6.192     G1V 212 0
38 * 4 Equ SB* 21 05 26.7036345960 +05 57 29.884406832       5.6   F8V 136 0
39 HD 200877 PM* 21 05 48.5376987480 +15 19 37.986084588 7.070 7.100 6.640     F7IV 36 0
40 HD 201891 Pe* 21 11 59.0321495469 +17 43 39.890919730 7.74 7.88 7.37 6.91 6.59 G5V_Fe-2.5 393 0
41 HD 204121 PM* 21 26 28.0527489888 +01 06 12.088012536       5.9   F5V 91 0
42 HD 208906 PM* 21 58 40.8320586106 +29 48 45.462564846 7.35 7.47 6.96 6.53 6.22 G0VmF2 174 0
43 * iot Peg SB* 22 07 00.6655101792 +25 20 42.356386464 4.190 4.200 3.770 3.36 3.11 F5V 443 1
44 HD 211976 * 22 20 55.7972067264 +08 11 12.271519068   6.621 6.163     F5V 99 0
45 * 33 Peg ** 22 23 39.5646960208 +20 50 53.839403909 6.690 6.690   5.9   F7IV 55 0
46 HD 213429 SB* 22 31 18.3282619654 -06 33 19.068890370   6.702 6.160     F8V 117 0
47 HD 219476 PM* 23 15 41.6669049360 +31 40 32.166561144       7.3   F8 42 0
48 HD 221356 PM* 23 31 31.5027738192 -04 05 14.650543968   7.03 6.49     F7V 164 0
49 * iot Psc PM* 23 39 57.0406036160 +05 37 34.653911951 4.640 4.620 4.120 3.68 3.37 F7V 617 0
50 HD 222872 PM* 23 44 29.0653971768 -26 14 47.883366276   6.70 6.23 7.43   F3/5V 31 0

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