As is well known in the theory of nonlinear differential equations, straightforward perturbation theory leads to approximate solutions with the wrong asymptotic behavior. We consider a real scalar field satifying the Klein-Gordon equation with a φ{symbol}3 self-current, in both the classical and second-quantized versions. We demonstrate that the usual, approximate solutions are asymptotically unbounded in both cases. We present a solution up to a normalization factor for the function or Heisenberg operator φ{symbol} to first order in the coupling with the correct asymptotic behavior. In the quantum case this forces one to introduce a q-number renormalized mass. The discussion is limited to solutions periodic in a finite box. A discussion of the wave-function renormalization and the limit of infinite box volume is deferred here. The method of approximation used is a generalization of standard techniques in the theory of nonlinear differential equations, and does not require adiabatic switching of the interaction. © 1969 Società Italiana di Fisica.