Quantum Field Perturbation Theory Revisited

Schwinger's formalism in quantum field theory can be easily implemented in the case of scalar theories in $D$ dimension with exponential interactions, such as $μ^D\exp(αϕ)$. In particular, we use the relation $\exp\big(α{δ\over δJ(x)}\big)\exp(-Z_0[J])=\exp(-Z_0[J+α_x])$ with $J$ the external source, and $α_x(y)=αδ(y-x)$. Such a shift is strictly related to the normal ordering of $\exp(αϕ)$ and to a scaling relation which follows by renormalizing $μ$. Next, we derive a new formulation of perturbation theory for the potentials $V(ϕ)={λ\over n!}:ϕ^n:$, using the generating functional associated to $:\exp(αϕ):$. The $Δ(0)$-terms related to the normal ordering are absorbed at once. The functional derivatives with respect to $J$ to compute the generating functional are replaced by ordinary derivatives with respect to auxiliary parameters. We focus on scalar theories, but the method is general and similar investigations extend to other theories.

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