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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Miscellaneous Exotica 547<br />

Table 15.1. Bounds on the present-day ĠN/G N . (Adapted from Will 1993.)<br />

Method Ġ N /G N References<br />

[10 −12 yr −1 ]<br />

L<strong>as</strong>er ranging (Moon) 0 ± 10 Müller et al. (1991)<br />

Radar ranging (Mars) −2 ± 10 Shapiro (1990)<br />

Binary pulsar 1913+16 11 ± 11 Damour and Taylor (1991)<br />

Spin-down PSR 0655+64 < 55 Goldman (1990)<br />

recent discussions have also addressed the possibility of an oscillating<br />

G N (Hill, Steinhardt, and Turner 1990; Accetta and Steinhardt 1991)<br />

with a rate of change much f<strong>as</strong>ter than H. The following discussion<br />

does not generically address such extreme model <strong>as</strong>sumptions.<br />

The G N rate of change can be tested by a detailed study of the<br />

orbits of celestial bodies. Particularly precise data exist in the solar<br />

system from l<strong>as</strong>er ranging of the moon and radar ranging of planets,<br />

notably by the Viking landers on Mars. Very precise orbital data<br />

also exist beginning 1974 <strong>for</strong> the binary pulsar PSR 1913+16; among<br />

other things its orbital decay reveals the emission of gravitational radiation.<br />

A weaker but also less model-dependent bound can be derived<br />

from the spin-down rate of the pulsar PSR 0655+64. These<br />

present-day limits on ĠN/G N are summarized in Tab. 15.1; altogether<br />

|ĠN/G N | < ∼ 20×10 −12 yr −1 is probably a safe limit. The Hubble expansion<br />

parameter today is H 0 = h 100 km s −1 Mpc −1 = h 1.02×10 −10 yr −1<br />

(observationally 0.4 < ∼ h < ∼ 1). Thus today |σ| < ∼ 0.2 h −1 .<br />

15.2.2 Big-Bang Nucleosynthesis<br />

An interesting constraint on the value of G N in the early universe arises<br />

from the observed primordial light element abundances <strong>as</strong> first discussed<br />

by Barrow (1978). 94 In a Friedman-Robertson-Walker model of<br />

the universe the expansion rate is given by H 2 = (Ṙ/R)2 = 8π 3 G N ρ<br />

in terms of the energy density ρ which, during the epoch of nucleosynthesis,<br />

is dominated by radiation (photons, neutrinos). It is a standard<br />

94 Apparently there is an earlier discussion of this limit by G. Steigman in an<br />

unpublished essay <strong>for</strong> the 1976 Gravity Research Foundation Awards. Subsequent<br />

refinements include Rothman and Matzner (1982), Accetta, Krauss, and<br />

Romanelli (1990), Damour and Gundlach (1991), and C<strong>as</strong><strong>as</strong>, García-Bellido, and<br />

Quirós (1992).

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