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Locally acting mirror Hamiltonians
Published in Journal of Modern Optics, 2021
Jake Southall, Daniel Hodgson, Robert Purdy, Almut Beige
Before analysing the dynamics associated with the mirror Hamiltonian in Equation (41), let us move from the Schrödinger into the interaction picture with respect to the free Hamiltonian and with respect to t = 0. In the following, denotes the state vector of the quantized EM field at time t in the interaction picture with being the corresponding state vector in the Schrödinger picture. As usual in physics, we define the state vector in the interaction picture such that
Taking the time derivative of the above equation, one can show that this state vector evolves according to a Schrödinger equation but with the corresponding Hamiltonian given by
In the absence of a mirror potential, at all times and local field excitations remain at their initial positions. The purpose of changing into the interaction picture is to simplify the following calculations by removing all free-space dynamics from the time evolution of the EM field.