We consider perturbative expansions in theories with an infrared cutof
f lambda. The infrared sensitive parts are defined as terms non-analyt
ic in infinitesimal lambda(2) and powers of this cutoff characterize t
he strength of these infrared contributions. It is argued that the sum
over the initial and final degenerate (as lambda --> 0) states, which
is required by the Kinoshita-Lee-Nauenberg theorem, eliminates terms
of order lambda(0) and lambda(1). However, the quadratic and higher or
der terms in general do not cancel. This is investigated using simple
examples of KLN cancellations, of relevance to the inclusive decay rat
e of a heavy particle, at the one loop level. (C) 1998 Elsevier Scienc
e B.V.