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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Chapter 15<br />

Miscellaneous Exotica<br />

Stellar-evolution constraints on a variety of hypotheses are discussed<br />

and compared with limits from other sources. Specifically, a possible<br />

time variation of Fermi’s and Newton’s constant, the validity of the<br />

equivalence principle, a photon m<strong>as</strong>s and charge, the existence of free<br />

quarks and supersymmetric particles, and the role of majorons and<br />

millicharged particles are considered.<br />

15.1 Constancy of Fermi’s Constant<br />

One of the b<strong>as</strong>ic physical <strong>as</strong>sumptions commonly made in <strong>as</strong>trophysical<br />

research is that the laws of nature are the same at different places<br />

in the universe, and at earlier times here and elsewhere. Apparently<br />

this <strong>as</strong>sumption h<strong>as</strong> never been challenged seriously by any experiment<br />

or observation that would have indicated a spatial or temporal variation<br />

of parameters such <strong>as</strong> particle m<strong>as</strong>ses or coupling constants. At<br />

the present time it is not known what fixes the values of such “fundamental<br />

numbers.” There<strong>for</strong>e, the possibility that they vary in time or<br />

space cannot be a priori rejected. Notably, Dirac (1937, 1938) is often<br />

quoted <strong>for</strong> his speculation that the large value of some dimensionless<br />

numbers occurring in physics are related to variations of some physical<br />

constants on cosmological time scales. Whatever the merit of Dirac’s<br />

large numbers hypothesis, it remains an interesting t<strong>as</strong>k to isolate simple<br />

observables that are sensitive to variations of certain “constants.”<br />

One instructive stellar-evolution example w<strong>as</strong> discussed by Scherrer<br />

and Spergel (1993) who considered the constancy of Fermi’s constant<br />

G F which governs weak-interaction physics. The particle-physics standard<br />

model gives G −1<br />

F = √ 2 Φ 2 0 in terms of the Higgs-field vacuum<br />

expectation value Φ 0 . Scherrer and Spergel noted that a nonconstant<br />

545

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