(abridged) Using the UH8K mosaic camera, we have measured the angular
correlation function \omega(\theta) for 100,000 galaxies over four widely
separated fields totalling ~1\deg^2 and reaching IAB~25.5. With this sample we
investigate the dependence of \omega(\theta) at 1', A_\omega(1'), on sample
median IAB magnitude in the range 19.5<I(AB-med)<24. Our results show that
A_\omega(1') decreases monotonically to IAB~25. At bright magnitudes,
\omega(\theta) is consistent with a power-law of slope \delta = -0.8 for
0.2'<\theta<3.0' but at fainter magnitudes we find \delta ~ -0.6. At the
3\sigma level, our observations are still consistent with \delta=-0.8.
Furthermore, in the magnitude ranges 18.5<IAB<24.0 and 18.5<IAB<23.0 we find
galaxies with 2.6<(V-I)AB<2.9 have A_\omega(1')'s which are ~10x higher than
field values. We demonstrate that our model redshift distributions for the
faint galaxy population are in good agreement with current spectroscopic
observations. Using these predictions, we find that for low-omega cosmologies
and assuming r_0=4.3/h Mpc, in the range 19.5<I(AB-med)<22, the growth of
galaxy clustering is \epsilon~0. However, at 22<I(AB-med)<24.0, our
observations are consistent with \epsilon>1. Models with \epsilon~0 cannot
simultaneously match both bright and faint measurements of A_\omega(1`). We
show how this result is a natural consequence of the ``bias-free'' nature of
the \epsilon formalism and is consistent with the field galaxy population in
the range 22.0<IAB<24.0 being dominated by galaxies of low intrinsic
luminosity.Comment: 20 pages, 21 figures, requires natbib.sty, accepted for publication
in Astronomy and Astrophysic