Abstract
We describe a quantum perturbative approach to evaluating the phase shift of an atom interferometer in a weakly anharmonic trap. This provides a simple way to evaluate quantum corrections to the standard semi-classical approximation. The calculation benefits from the use of generalized coherent states for a basis. We find that the form of the semi-classical approximation remains valid to first order in the anharmonic perturbation, but that phase differences arise because the trajectory of a quantum wave packet will generally deviate from that of a classical particle. The quantum correction to the phase is a factor ℓ²/A² smaller than the semi-classical perturbation itself, where ℓ is the quantum harmonic oscillator length scale and A is the classical amplitude of the motion. We provide analytical results for one-dimensional perturbations of power three through six in the position coordinate.