Estimates on Functional Integrals of Quantum Mechanics and Non-Relativistic Quantum Field Theory

Abstract

We provide a unified method for obtaining upper bounds for certain functional integrals appearing in quantum mechanics and non-relativistic quantum field theory, functionals of the form $E\left[\exp (A_T)\right]$, the (effective) action $A_T$ being a function of particle trajectories up to time $T$. The estimates in turn yield rigorous lower bounds for ground state energies, via the Feynman-Kac formula. The upper bounds are obtained by writing the action for these functional integrals in terms of stochastic integrals. The method is first illustrated in familiar quantum mechanical settings: for the hydrogen atom, for a Schrödinger operator with $1/|x{|}^2$ potential with small coupling, and, with a modest adaptation of the method, for the harmonic oscillator. We then present our principal applications of the method, in the settings of non-relativistic quantum field theories for particles moving in a quantized Bose field, including the optical polaron and Nelson models.

References in corpus (1)

• Erratum: Exact Ground State Energy of the Strong-Coupling Polaron

Cited by in corpus (1)

• Feynman-Kac formulas for the ultra-violet renormalized Nelson model