The peculiar velocities of galaxies distort the pattern of galaxy clustering in redshift space, making the redshift-space power spectrum anisotropic. In the linear regime of gravitational instability models, the strength of this distortion depends only on the ratio |β≡ f(Ω)/b≈Ω0.6/b|, where Ω is the cosmological density parameter, and b is the bias parameter. We derive a linear-theory estimator for β, based on the harmonic moments of the redshift-space power spectrum. Using N-body simulations, we examine the impact of non-linear gravitational clustering on the power-spectrum anisotropy and on our β-estimator. Non-linear effects can be important out to wavelengths |λ~50 h⁻¹| Mpc or larger; in most cases, they lower the quadrupole moment of the power spectrum, and thereby depress the estimate of β below the true value. With a sufficiently large redshift survey, the scaling of non-linear effects may allow separate determinations of Ω and b. We describe a practical technique for measuring the anisotropy of the power spectrum from galaxy redshift surveys, and we test the technique on mock catalogues drawn from the N-body simulations. Preliminary application of our methods to the 1.2-Jy IRAS galaxy survey yields |βₑst~ 0.3-0.4| at wavelengths |λ~30-40 h⁻¹| Mpc. Non-linear effects remain important at these scales, so this estimate of β is probably lower than the true value.
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Cole et al. (1994) studied this question.