We report on a numerical study of the spherically symmetric collapse o
f a self-gravitating massless scalar field. Earlier results of Choptui
k (1992, 1994) are confirmed. The field either disperses to infinity o
r collapses to a black hole, depending on the strength of the initial
data. For evolutions where the strength is close to but below the stre
ngth required to form a black hole, we argue that there will be a regi
on close to the axis where the scalar curvature and field energy densi
ty can reach arbitrarily large levels, and which is visible to distant
observers.