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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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62 Chapter 2<br />

f<strong>as</strong>t. There<strong>for</strong>e, the stars along the red-giant branch (RGB), horizontal<br />

branch (HB), and <strong>as</strong>ymptotic giant branch (AGB) in a globular<br />

cluster have almost identical initial m<strong>as</strong>ses whence <strong>for</strong> these ph<strong>as</strong>es a<br />

single-star track is practically identical with an isochrone. On the other<br />

hand, the TO region requires the construction of detailed theoretical<br />

isochrones to compare theory and observations and thus to determine<br />

the ages of globular clusters.<br />

In order to <strong>as</strong>sociate a certain stellar m<strong>as</strong>s with the TO in a cluster<br />

one needs to know the absolute brightness of the stars at the TO, i.e.<br />

one needs to know the precise distance. All else being equal, the inferred<br />

age varies with the TO luminosity <strong>as</strong> ∂ log(age)/∂ log L TO = −0.85 or<br />

∂ log(age)/∂V TO = 0.34 (Iben and Renzini 1984). There<strong>for</strong>e, a 0.1 mag<br />

error in V TO leads to an 8% uncertainty in the inferred cluster age.<br />

Put another way, because L ∝ (distance) 2 a 10% uncertainty in cluster<br />

distances leads to an 18% age uncertainty. This is the main problem<br />

with the age determination of globular clusters.<br />

A particularly useful method to me<strong>as</strong>ure the distance is to use<br />

RR Lyrae stars <strong>as</strong> standard candles. As discussed in Sect. 2.1, their<br />

luminosity is determined almost entirely by their core m<strong>as</strong>s (apart from<br />

a dependence on chemical composition), which in turn is fixed by helium<br />

ignition on the RGB which, again, depends only on the chemical<br />

composition and not on the red-giant envelope m<strong>as</strong>s. There<strong>for</strong>e, the<br />

brightness of the HB is nearly independent of stellar m<strong>as</strong>s. Consequently,<br />

the brightness difference ∆VHB<br />

TO between the HB and the TO<br />

is a distance-independent me<strong>as</strong>ure of the TO m<strong>as</strong>s and thus of the cluster<br />

age. Moreover, because the color of RR Lyrae stars coincides with<br />

that of the TO region it is not necessary to convert from the me<strong>as</strong>ured<br />

brightness with a certain filter (e.g. visual brightness V ) to a bolometric<br />

brightness, i.e. there is no need <strong>for</strong> a bolometric correction (BC).<br />

Also, RR Lyrae stars are bright and e<strong>as</strong>ily identified because of their<br />

pulsations. There<strong>for</strong>e, ∆VHB<br />

TO is one of the most important observables<br />

in the color-magnitude diagram of globular clusters (Iben and Renzini<br />

1984; Sandage 1986).<br />

As an example the recent ∆VHB<br />

TO<br />

determinations of Buonanno, Corsi,<br />

and Fusi Pecci (1989) in 19 globular cluster are shown in Fig. 2.17 <strong>as</strong><br />

a function of metallicity; the logarithmic metallicity me<strong>as</strong>ure [Fe/H] is<br />

defined in Eq. (2.15). The best linear fit is<br />

∆V TO<br />

HB = (3.54 ± 0.13) − (0.008 ± 0.078) [Fe/H], (2.13)<br />

so that the HB brightness varies with metallicity almost exactly <strong>as</strong> the<br />

TO brightness. The me<strong>as</strong>ured points are in agreement with a Gaussian

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