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 79<br />

into question in recent years (e.g. Wheeler, Sneden, and Truran 1989).<br />

It is thought that in these systems the “α elements” (mostly oxygen)<br />

are enhanced relative to iron. RG sequences calculated by Raffelt and<br />

Weiss (1992) with somewhat extreme α enhancements indicated that<br />

the red-giant core m<strong>as</strong>s and luminosity at the helium fl<strong>as</strong>h are only<br />

moderately changed. Most of the change that did occur w<strong>as</strong> due to<br />

the reduction of Fe at constant Z because of the α enhancement. Put<br />

another way, if Z 13 = [Fe/H] + 1.3 is used <strong>as</strong> the defining equation <strong>for</strong><br />

the above “reduced metallicity” the effect of α enhancements appear<br />

to be rather minimal.<br />

Catelan, de Freit<strong>as</strong> Pacheco, and Horvath (1995) have taken the<br />

point of view that <strong>for</strong> enhanced α elements one should rescale the<br />

metallicity according to a recipe given by Chieffi, Straniero, and Salaris<br />

(1991). Put another way, the metallicity parameter of Eq. (2.16) that<br />

w<strong>as</strong> used in the previous sections should be redefined <strong>as</strong><br />

Z 13 ≡ [Fe/H] + 1.3 + log(0.579 f + 0.421). (2.39)<br />

Here, f is the enhancement factor of the abundance of α elements<br />

relative to the solar value. For f = 3 one finds that Z 13 must be<br />

offset by +0.33. Catelan, de Freit<strong>as</strong> Pacheco, and Horvath (1995) went<br />

through their analysis with this modification, causing the allowed bands<br />

of Fig. 2.23 to be slightly shifted relative to each other. However, the<br />

overall change is small, well within the stated upper limit on δM c .<br />

In summary, no effect h<strong>as</strong> been discussed in the literature that would<br />

cause the predicted core m<strong>as</strong>s at helium ignition to deviate from its<br />

standard value beyond the adopted limit of ±0.025 M ⊙ . There<strong>for</strong>e, any<br />

new energy-loss mechanism that would cause a significantly larger corem<strong>as</strong>s<br />

excess would have to be compensated by a hitherto unidentified<br />

other novel effect.<br />

2.5 Particle Bounds from Globular-Cluster <strong>Stars</strong><br />

2.5.1 Helium-Burning Lifetime<br />

A particularly simple argument to constrain the properties of novel<br />

particles arises from the observed duration of helium burning of lowm<strong>as</strong>s<br />

stars, i.e. <strong>for</strong>m the lifetime of stars on the horizontal branch (HB).<br />

In Sect. 2.4.4 it w<strong>as</strong> argued that the number ratio R of stars on the HB<br />

vs. RGB in globular clusters agreed with standard predictions to within<br />

10%. There<strong>for</strong>e, the helium-burning lifetime t He agrees with standard<br />

predictions to within this limit. A less significant confirmation arises

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

Saved successfully!

Ooh no, something went wrong!