We propose a semiclassical approach to calculate multiparticle cross s
ections in scalar theories, which have been strongly argued to have th
e exponential form exp(lambda(-1) F(lambda n, epsilon)) in the regime
lambda --> 0, lambda n, epsilon = fixed, where lambda is the scalar co
upling, n is the number of produced particles, and epsilon is the kine
tic energy per final particle. The formalism is based on singular solu
tions to the field equation, which satisfy certain boundary and extrem
izing conditions. At low multiplicities and small kinetic energies per
final particle we reproduce in the framework of this formalism the ma
in perturbative results. We also obtain a fewer bound on the tree-leve
l cross section in the ultra-relativistic regime.