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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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66 Chapter 2<br />

a) Composition Parameters<br />

The chemical composition is characterized by the helium content and<br />

the metallicity. The convective envelope on the RGB at some point<br />

reaches down into the region of a variable composition profile caused<br />

by nuclear burning, causing a certain amount of processed material<br />

(helium) to be dredged up. There<strong>for</strong>e, the helium m<strong>as</strong>s fraction Y env<br />

of the envelope is slightly larger than the value Y at <strong>for</strong>mation. The<br />

amount of dredge-up is approximately given by (Sweigart, Renzini, and<br />

Tornambé 1987)<br />

∆Y s ≡ Y env − Y ≈ 0.0136 + 0.0055 Z 13 , (2.14)<br />

where the metallicity parameter Z 13 is defined in Eq. (2.16) below.<br />

However, because the exact amount of convective dredge-up is somewhat<br />

model dependent, and because me<strong>as</strong>urements of 12 C/ 13 C ratios<br />

in metal-poor field red giants seem to indicate that the dredge-up of<br />

processed material is more efficient than predicted by standard calculations<br />

(Sneden, Pilachewski, and VandenBerg 1986) it is best to use Y env<br />

rather than Y <strong>as</strong> an independent parameter to characterize red giants<br />

and HB stars. 10<br />

Gravitational settling of helium throughout the MS evolution h<strong>as</strong><br />

the opposite effect of reducing the envelope abundance relative to the<br />

initial homogeneous value. In recent evolutionary sequences which were<br />

calculated to estimate the effect of helium diffusion on the inferred<br />

globular-cluster ages a decre<strong>as</strong>e between ∆Y s = −0.009 and −0.015 w<strong>as</strong><br />

found (Proffitt and Michaud 1991; Chaboyer et al. 1992). There<strong>for</strong>e,<br />

the effect of MS gravitational settling and that of RG convective dredgeup<br />

appear to cancel each other more or less so that Y env appears to be<br />

much closer to the initial value Y than had been thought previously.<br />

The metallicity is usually characterized by the m<strong>as</strong>s fraction Z of<br />

elements heavier than helium. Because iron is most important <strong>for</strong> the<br />

opacities one often uses the abundance of iron relative to hydrogen<br />

<strong>as</strong> a metallicity me<strong>as</strong>ure. It is characterized by the quantity [Fe/H]<br />

which is the logarithmic abundance of iron over hydrogen relative to<br />

the solar value. If the solar metallicity is taken to be Z ⊙ = 0.02 so that<br />

10 In their calculation of RG sequences, Sweigart and Gross (1978) used the symbol<br />

Y to denote the MS helium abundance; the envelope abundance near the helium<br />

fl<strong>as</strong>h can be inferred from their tabulation of ∆Y s values <strong>for</strong> each sequence. In<br />

their 1976 study of HB sequences, they used the symbol Y to denote the envelope<br />

abundance which is here consistently called Y env .

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