28.01.2015 Views

Stars as Laboratories for Fundamental Physics - MPP Theory Group

Stars as Laboratories for Fundamental Physics - MPP Theory Group

Stars as Laboratories for Fundamental Physics - MPP Theory Group

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Anomalous Stellar Energy Losses Bounded by Observations 65<br />

A very important me<strong>as</strong>ure of the speed of evolution of a single star<br />

along the RGB, HB, and AGB is the relative number of stars found on<br />

these branches in a given cluster. Because <strong>for</strong> these advanced evolutionary<br />

ph<strong>as</strong>es a single-star track is essentially an isochrone, these number<br />

ratios R give us directly the relative amounts of time spent on these<br />

branches (“R-method”). For example, a novel energy-loss mechanism<br />

that operates mostly in the nondegenerate core of an HB star would<br />

shorten the helium-burning lifetime. This possibility is constrained by<br />

the relative number of stars found on the HB and RGB where the RGB<br />

in this context refers to that part which is brighter than the HB.<br />

When a star <strong>as</strong>cends the RGB, its hydrogen-burning shell encounters<br />

at some point a discontinuity in the composition profile left behind<br />

by a previous deep penetration of the envelope convection into the<br />

region of varying hydrogen content caused by nuclear burning. The <strong>as</strong>cent<br />

is briefly interrupted and the star stays at a fixed luminosity <strong>for</strong> a<br />

brief period of time. Afterward, the hydrogen shell works itself through<br />

a constant composition profile which w<strong>as</strong> prepared by the convective<br />

envelope. There<strong>for</strong>e, at a brightness near the HB one expects to find<br />

a “bump” in the number of stars on the RGB, i.e. in the distribution<br />

∂N/∂M bol which essentially corresponds to dt/dM bol <strong>for</strong> a single-star<br />

evolutionary track (Fig. 2.18). The bump w<strong>as</strong> recently identified in a<br />

number of clusters; <strong>for</strong> a particularly beautiful example see Fig. 2.19.<br />

It h<strong>as</strong> been suggested to use it <strong>as</strong> a standard candle to calibrate the<br />

RR Lyrae brightness-metallicity relation (Fusi Pecci et al. 1990).<br />

An important observable is the absolute brightness of RR Lyrae<br />

stars which are not members of globular clusters. No re<strong>as</strong>on is known<br />

why these field stars <strong>for</strong> a given metallicity should be any different from<br />

those found in a cluster and so brightness determinations of nearby<br />

RR Lyrae stars provide important in<strong>for</strong>mation about their luminosity<br />

calibration.<br />

2.4.2 Theoretical Relations<br />

In order to test the standard stellar-evolution picture against the observables<br />

introduced in Sect. 2.4.1 they need to be related to stellar<br />

properties such <strong>as</strong> m<strong>as</strong>s and chemical composition. In the p<strong>as</strong>t, extensive<br />

grids of stellar evolutionary sequences have been calculated and<br />

have been used to derive analytic approximations <strong>for</strong> the connection<br />

between various stellar parameters; <strong>as</strong> a canonical standard I use the<br />

evolutionary HB and RG sequences of Sweigart and Gross (1976, 1978).

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!