Starting from a general material system of
NN
particles coupled to a cavity, we use a coherent-state path integral
formulation to produce a effective theory for the material degrees of
freedom. We tackle the effects of image charges, the
A^2A2
term and a multimode arbitrary-geometry cavity. The resulting
(non-local) action has the photonic degrees of freedom replaced by an
effective position-dependent interaction between the particles. In the
large-NN
limit, we discuss how the theory can be cast into an effective
Hamiltonian where the cavity induced interactions are made explicit.
The theory is applicable, beyond cavity QED, to any system where bulk
material is linearly coupled to a diagonalizable bosonic bath. We
highlight the differences of the theory with other well-known methods
and numerically study its finite-size scaling on the Dicke model.
Finally, we showcase its descriptive power with three examples: photon
condensation, the 2D free electron gas in a cavity and the modification
of magnetic interactions between molecular spins; recovering, condensing
and extending some recent results in the literature.