1986
DOI: 10.1086/131781
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On the carbon abundance of subgiant stars in the globular cluster M 92

Abstract: We find that <[C/Fe]> ~ 0.0 in stars at the base of the subgiant branch and approaches +0.1 in stars near the main-sequence turnoff in the metal-poor globular cluster M 92. The carbon abundance falls on the average by about 0.5 dex by the time stars reach My -hi.5. These carbon depletions occur early enough and are approximately the right size to account for the large average nitrogen enhancement ([N/Fe] ~ +0.65) observed by Carbon et al. (1982) in M 92 subgiants near My -hi .5. Although the present observatio… Show more

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Cited by 73 publications
(83 citation statements)
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“…However, a close inspection of the data does suggest that there might be a slight peak on the subgiant branch, as indeed Fukuoka and Simoda make the comment that "the only meaningful deviation may be a bump at V ~ 18". Curiously, this is very close to where Langer et al (1986) find the depletion in the surface 12 C abundance in M 92 stars to begin. But, if there truly is a peak in the observed luminosity function at about this magnitude (M v ~ 3.3), it is a very subtle feature.…”
Section: A Abundance Changes In Standard Modelssupporting
confidence: 62%
See 1 more Smart Citation
“…However, a close inspection of the data does suggest that there might be a slight peak on the subgiant branch, as indeed Fukuoka and Simoda make the comment that "the only meaningful deviation may be a bump at V ~ 18". Curiously, this is very close to where Langer et al (1986) find the depletion in the surface 12 C abundance in M 92 stars to begin. But, if there truly is a peak in the observed luminosity function at about this magnitude (M v ~ 3.3), it is a very subtle feature.…”
Section: A Abundance Changes In Standard Modelssupporting
confidence: 62%
“…Is it possible to construct partially-mixed main-sequence models which can explain the observed abundances without violating other constraints from the data? Second, the change in C abundance which is seen along the giant branch in systems like M 92 (Langer et al 1986) suggests that deep mixing in this case commences near the base of Post-ZAMS Models Within the mathematical framework of the stellar evolution code used for the present calculations, it is possible to arbitrarily homogenize any region of a model and to follow its evolution. This provides a means by which mixing at different evolutionary stages, and to different depths, can be experimented with in order to search for potential mixing histories that could produce the cluster abundance inhomogeneities.…”
Section: A Abundance Changes In Standard Modelsmentioning
confidence: 99%
“…In giants it is possible that material from deep layers, where carbon is converted into nitrogen, has been brought to the surface during previous mixing episodes. This phenomenon is well known in globular cluster stars (e.g., Langer et al 1986;Kraft 1994). To check for this effect, Fig.…”
Section: Cs 22948-066mentioning
confidence: 78%
“…We were able to estimate values of [C/Fe] and [N/Fe], and show that, in M92 at least, although wide variations in these abundances could be found at any given location in the HR diagram, on the average [C/Fe] fell by a factor of 10 as stars progressed from the main sequence to the tip of the giant branch , indicating that the external stellar layers had been processed by convective mixing to regions in or near the hydrogen-burning shell. Stars near the main sequence had to be observed using the Palomar 200-inch telescope, thanks to an observing run with Bev Oke (Langer et al 1986). Suntzeff's thesis (1981) dealt with M3 and M13, for which similar variations were found at a given luminosity, but in which the systematic decline with luminosity in mean carbon abundance was not so clearly indicated.…”
Section: Globular Cluster Carbon and Nitrogen Abundances-syntheticmentioning
confidence: 99%