Abstract
The "zero-mass" limiting short-distance theory for the gφ4 interaction is explicitly constructed. The propagator is computed to third order and the vertex to fourth order in g, the zero-mass coupling constant. The Gell-Mann and Low short-distance equations which result as exact consequences can be explicitly determined to all orders in perturbation theory. If the eigenvalue condition is imposed, one can construct a theory in terms of the massless free propagator and a conformal-invariant four-point vertex function only. The energy-momentum tensor of this theory is the same as that proposed by Callan, Coleman, and Jackiw.