We construct a quantum theory of light in nonlinearly responding materials with dispersion
and absorption and, in particular, show the emergence of non-Gaussian noise associated with
nonlinear absorption processes. Our theory is based on a path-integral formulation of the
microscopic Huttner-Barnett model including cubic matter self-interaction required for
χ(2) nonlinear processes. We show that the noise polarization emerges naturally from
a decoupling of the stochastic weights of the bath response which, in case of cubic
self-interactions, leads to a decoupling via Airy functions. As the theory is, by
construction, consistent with the nonlinear fluctuation-dissipation theorem, it constitutes
a viable quantum theory of light in nonlinear media.
We present a canonical quantum theory of radiation in nonlinear media taking into account the effects of linear dispersion and absorption in a consistent way. We start from a microscopic model and apply recently developed concepts of the quantization of radiation in dispersive and absorbing linear media and extend the theory in order to include nonlinear optical processes. We derive propagation equations in space and time for the quantized radiation field, with special emphasis on the propagation of quantum-light pulses in Kerr media. In particular, the method enables us to derive systematically the noise sources that arise naturally in the nonlinear terms.
We construct a quantum theory of light in nonlinear dielectric media with dispersion and absorption. We employ a mesoscopic model for the light-matter interaction that include a fourth-order nonlinearity in the material response. Quantization is performed by constructing an effective action in a path-integral formalism by integrating out matter and bath degrees of freedom. We show how a nonlinear response function associated with Kerr nonlinearity is obtained through the model and, after full field quantization, we derive the Feynman rules from this theory.