We show that phase transitions occur in the confined growth of chains forme
d by self-avoiding hard spheres. Planar growth arises from the stochastic i
nterplay of two simple opposing mechanisms: enforced connectivity and self-
avoidance between spheres. Depending on the value of parameter T that sets
the tendency of growth along a definite direction, the structures either se
ttle into a box-limited or a self-trapped configuration. We established tha
t a T value exists where fully grown structures are likely to be bigger for
the same confinement area. The said T value is independent of confinement
area for sufficiently large boxes and it is near a critical point for a pha
se transition between the box-limited configuration and the self-trapped co
nfiguration. (C) 2000 Elsevier Science B.V. All rights reserved.