1999ApJ...523..654R


Query : 1999ApJ...523..654R

1999ApJ...523..654R - Astrophys. J., 523, 654-677 (1999/October-1)

The Spite lithium plateau: ultrathin but postprimordial.

RYAN S.G., NORRIS J.E. and BEERS T.C.

Abstract (from CDS):

We have studied 23 very metal-poor field turnoff stars, specifically chosen to enable a precise measurement of the dispersion in the lithium abundance of the Spite Li plateau. We concentrated on stars having a narrow range of effective temperature and very low metallicities ([Fe/H]≲-2.5) to reduce the effects of systematic errors and have made particular efforts to minimize random errors. A typical statistical error for our abundances is 0.033 dex (1 σ), which represents a factor of 2 improvement on most previous studies. Our sample does not exhibit a trend with effective temperature, although the temperature range is limited. However, for -3.6<[Fe/H]←2.3 we do recover a dependence on metallicity at dA(Li)/d[Fe/H]=0.118±0.023 (1 σ) dex per dex, almost the same level as discussed previously. Earlier claims for a lack of dependence of A(Li) on abundance are shown to have arisen probably from noisier estimates of effective temperatures and metallicities, which have erased the real trend. The dependence is concordant with theoretical predictions of Galactic chemical evolution (GCE) of Li (even in such metal-poor stars) and with the published level of 6Li in two of the stars of our sample, which we use to infer the GCE 7Li contribution. One of the 23 stars, G186-26, was known already to be strongly Li-depleted. Of the remaining 22 objects, 21 have abundances consistent with an observed spread about the metallicity trend of a mere 0.031 dex (1 σ). Because the formal errors are 0.033 dex, we conclude that the intrinsic spread is effectively zero at the very metal-poor halo turnoff. This is established at much higher precision than previous studies (∼0.06-0.08 dex). The essentially zero intrinsic spread leads to the conclusion that either these stars have all changed their surface Li abundances very uniformly, or else they exhibit close to the primordial abundance sought for its cosmological significance. We cannot rule out a uniform depletion mechanism, but economy of hypothesis supports the latter interpretation. The lack of spread in the A(Li) abundances limits permissible depletion by rotationally induced mixing models to less than 0.1 dex. Correcting for the GCE contribution to both 6Li and 7Li, we infer a primordial abundance A(Li)p≃2.00 dex, with three systematic uncertainties of up to 0.1 dex each depending on uncertainties in the effective temperature scale, stellar atmosphere models, and correction for GCE. (This value rests on an effective-temperature zero-point set by Magain's and Bell & Oke's b-y calibrations of metal-poor stars and the model atmospheres without convective overshoot.) We predict that observations of Li in extremely low-metallicity stars, having [Fe/H]←3, will yield smaller A(Li) values than the bulk of stars in this sample, consistent with a low primordial abundance. The difference between our field star observations and published M92 data suggests real field-to-cluster differences. This may indicate different angular momentum evolutionary histories, with interactions between protostellar disks in the dense globular cluster environments possibly being responsible. Further study of Li in globular clusters and in very metal-poor field samples is required to clarify the situation.

Abstract Copyright:

Journal keyword(s): Galaxy: Halo - Nuclear Reactions, Nucleosynthesis, Abundances - stars: abundances - stars: Population II

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 - 2024
#notes
1 LP 651-4 PM* 02 44 11.7179917488 -05 27 00.003085992   12.35 11.97     ~ 25 0
2 G 4-37 Pe* 02 44 35.0876406984 +08 28 50.094009408   11.90 11.4 11.0   F7 84 0
3 LP 831-70 PM* 03 06 05.4386096664 -22 19 17.828964660   11.97 11.80     ~ 48 0
4 CD-33 1173 Pe* 03 19 35.3159594880 -32 50 43.157572008   11.272 10.902 10.421 10.152 CEMP 58 0
5 BD+03 740 HB* 05 01 16.6226363256 +04 06 37.021736844 9.97 10.17 9.7 9.6   sdF0 174 0
6 BD+24 1676 Pe* 07 30 41.2662525096 +24 05 10.248524088   11.15 10.7 10.4   F 129 0
7 BD+20 2030 SB* 08 16 07.3522203887 +19 41 51.430977726   11.556 11.189 10.909 10.632 sdF0 51 0
8 HD 74000 Pe* 08 40 50.8036114756 -16 20 42.516208237 9.84 10.09 9.66     F2 270 0
9 BD+09 2190 Pe* 09 29 15.5615542183 +08 38 00.467004388   11.54   10.8   sdA5 133 0
10 Ross 889 Pe* 09 40 43.2053340378 +01 00 29.511836741       10.39   sdA4 160 0
11 HD 84937 Pe* 09 48 56.0992891997 +13 44 39.326709913 8.49 8.68 8.32 7.97 7.70 F8Vm-5 795 0
12 BD-13 3442 Pe* 11 46 50.6525751264 -14 06 43.458063768   10.662 10.274     CEMP 107 0
13 Wolf 1492 Pe* 13 40 02.4921849768 -00 02 18.750053436 11.601 11.832 11.451 11.184 10.892 sdF0: 284 0
14 Ross 841 Pe* 14 02 30.0900761861 -05 39 05.181979951   11.508 11.149 10.866 10.576 sdA3 151 0
15 BD+26 2621 Pe* 14 54 10.7123241110 +25 33 48.927279437   11.40 10.9 10.7   F0 46 0
16 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 938 0
17 CD-71 1234 Pe* 16 07 44.6410532021 -71 21 01.360284611   10.81 10.44     ~ 39 0
18 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2117 0
19 HD 160617 Pe* 17 42 49.3234249010 -40 19 15.503834657   9.18 8.7 8.394 8.065 G0 204 0
20 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2002 0
21 HD 338529 PM* 19 32 31.9104668184 +26 23 26.117367216   9.72   9.2   B5 207 0
22 HD 345957 PM* 20 10 48.1625876064 +23 57 54.510596568   9.36   8.6   G0V: 143 0
23 HD 340279 Pe* 20 24 45.4125969504 +25 03 07.109969040   11.23 10.8 10.7   A5 103 0
24 LP 635-14 Pe* 20 26 46.8302881512 -00 37 15.175129512 11.57 11.76 11.33     OB- 41 0
25 BPS CS 22943-0095 Pe* 20 27 29.9870188056 -46 50 56.315093100 11.857 12.063 12.62     ~ 24 0
26 LP 815-43 Pe* 20 38 13.2998605176 -20 26 10.850795808   11.31 10.72     ~ 76 0
27 CD-35 14849 PM* 21 33 49.7524989129 -35 26 14.228198341   10.95 10.56 10.59   B8 72 0
28 G 126-52 PM* 22 04 13.3810303392 +19 32 54.335372892       10.7   sd:F2 37 0
29 CD-24 17504 Pe* 23 07 20.2534619736 -23 52 35.954286096   12.51 12.18     CEMP-no 86 0

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