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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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554 Chapter 15<br />

Actually, a certain reduction of the true globular-cluster ages relative<br />

to their apparent ones would be a welcome cosmological effect <strong>as</strong><br />

they are, at best, marginally compatible with other cosmic age indicators.<br />

In view of the current limits on ĠN/G N summarized in Fig. 15.2<br />

this possibility cannot be excluded at present.<br />

15.3 Test of the Equivalence Principle<br />

The equivalence principle of Einstein’s general theory of relativity implies<br />

that the space-time trajectories of relativistic particles should be<br />

independent of internal degrees of freedom such <strong>as</strong> spin or flavor, and<br />

independent of the type of particle under consideration (photons, neutrinos).<br />

A number of <strong>as</strong>tronomical observations allow one to test this<br />

prediction. Laboratory tests of various consequences of the equivalence<br />

principle are discussed in Will’s (1993) book.<br />

Nonsymmetric extensions of general relativity (e.g. Moffat 1991)<br />

predict that different polarization components of electromagnetic waves<br />

propagate with different ph<strong>as</strong>e velocities in gravitational fields. This<br />

birefringence effect would lead to the depolarization of the Zeeman<br />

components of spectral lines emitted in magnetically active regions of<br />

the Sun. The absence of this depolarization effect leads to significant<br />

constraints on Moffat’s theory and others (Gabriel et al. 1991).<br />

In a similar approach one uses the difference of the Shapiro time<br />

delay between different particles or between different polarization states<br />

of a given particle which propagate through the same gravitational<br />

field. In Sect. 13.3 the absence of an anomalous shift between the<br />

SN 1987A photon and neutrino arrival times gave limits on violations<br />

of the equivalence principle because both pulses moved through the<br />

same galactic gravitational potential.<br />

Also, one may search <strong>for</strong> differences in the arrival times of leftand<br />

right-handed polarized electromagnetic signals from distant pulsars<br />

(LoSecco et al. 1989). The best bound w<strong>as</strong> obtained from an analysis of<br />

the pulse arrival times from PSR 1937+21 which is about 2.5 kpc away<br />

from Earth. One may write the effective gravitational potential in the<br />

<strong>for</strong>m V (r) = V 0 (r) [1 + A 1 σ ·ˆr + A 2 σ · v + A 3ˆr · (v × σ)] where r, v, and<br />

σ represent the location, velocity, and spin of the particles (photons,<br />

neutrinos). The PSR 1937+21 data then yield a constraint |A 1 | <<br />

4×10 −12 and |A 2 | < 1×10 −12 (Klein and Thorsett 1990), apparently<br />

the most restrictive limits of their kind.

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