The two-point angular correlation function of galaxies, omega(theta),
has been computed on equatorial fields observed with the Cerro Telolo
Inter-American Observatory 4 m prime focus, within a total area of 2,3
1 deg(2). In the magnitude range 19 less than or equal to m(R) less th
an or equal to 21.5, corresponding to (z) approximate to 0.35, we find
an excess of power in omega(theta) at scales 2 '' less than or equal
to theta less than or equal to 6 '' over what would be expected from a
n extrapolation of omega(theta) measured at larger theta. The signific
ance of this excess is approximate to 5 sigma. At larger scales, 6 ''
< theta less than or equal to 24 '' the amplitude of omega(theta) is 1
.6 times smaller than the standard nonevolutionary model. At these sca
les there is remarkable agreement between the present data and Infante
& Pritchet (1995). At large angular scales (6 '' < theta less than or
equal to 24 '') the data are best described by a model where clusteri
ng evolution in xi(r, z) has taken place. Strong luminosity evolution
cannot be ruled out with the present data. At smaller scales, 2 '' les
s than or equal to theta less than or equal to 6 '', our data are form
ally fitted by models where epsilon = -2.4(Omega = 0.2, r(0) = 5.1 h(-
1) Mpc) or r(0) 7.3 h(-1) Mpc (Omega = 0.2, epsilon = 0). If the mean
redshift of our sample is 0.35, then our data show a clear detection o
f the scale (approximate to 19 h(-1) kpc) where the clustering evoluti
on approaches a highly nonlinear regime, i.e., epsilon less than or eq
ual to 0. The rate at which galaxies merge has been computed. If this
rate is proportional to (1 + z)(m), then m = 2.2 +/- 0.5.