Radiative corrections in a nonlocal field theory
We extend the notion of a scalar field [Formula: see text] to that of a field Φ(Xμ(σ)) so that the space-time point Xμ(σ) depends on a parameter [Formula: see text]. A straightforward generalization of the [Formula: see text] interaction is considered (viz: a [Formula: see text] theory). Radiative corrections in both cases can be evaluated using a technique involving quantum mechanical path integrals. For the [Formula: see text] model, this involves the classical Lagrange density [Formula: see text] (viz: that of a particle in the "proper time gauge") while for the [Formula: see text] model the Lagrange density [Formula: see text] (viz: that of a string in the "conformai gauge") must be considered. The two-point function is examined in both cases.