Operator equation in a path integral 2026-10-24
An operator equation in a path integral asserts that insertions of vanish in every time-ordered correlation function with the other insertion points separated from . Derivatives of time ordering can produce Ward identity contact terms at coincidence. For example, conservation of a Dirac current gives a vanishing separated-point divergence, while a charged insertion contributes a delta-function contact term fixed by its transformation. A vanishing one-point expectation value alone is insufficient.
An operator equation in a path integral means that insertion of into every time-ordered correlation function vanishes when is separated from the other insertion points. At coincident points, Ward identity contact terms can remain; an operator equation does not assert that these distributions vanish.
Let be a product of local insertions. Make the local phase change of integration variables from part b. The functional measure has unit functional Jacobian: the opposite phases of and cancel in a vector-symmetry-preserving regularization in quantum field theory. There is no vector gauge anomaly. Invariance under a change of integration variables givesIf and , comparison of the coefficients of the arbitrary yields the Ward-Takahashi identityConsequently is an operator equation at separated points. This is stronger than just . For example, has , , so its two Ward identity contact terms are ; dropping them would give a false identity. Equivalently, the Dirac equation and the adjoint Dirac equation give , with the same coincident-point qualification in time-ordered correlation functions.