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This research establishes a rigorous quantization framework for open electromagnetic systems by deriving reservoirs directly from the dissipation geometry of the Maxwell operator, eliminating the need for phenomenological assumptions. By factoring the imaginary part of the operator, the method cleanly separates fluctuation channels into material absorption and boundary-assisted modes, enabling frequency-dependent scattering and noise kernels without relying on Markov or single-mode approximations. The approach offers significant theoretical utility for modeling complex photonic integrated circuits and lossy structures with arbitrary passive boundary conditions.
Dissipative Channels Determine Open Electromagnetic Quantization
arXiv:2606.08557v1 Announce Type: new Abstract: We formulate a quantization scheme for open electromagnetic systems with arbitrary passive boundary conditions. Rather than specifying reservoirs phenomenologically, the method identifies them from the dissipation geometry of the Maxwell operator. Factoring the imaginary part of the Maxwell operator gives a bosonic realization of the field operator and separates the fluctuation channels into medium-assisted reservoirs from material absorption and boundary-assisted reservoirs from exchange through the open boundary. Depending on the boundary condition, the latter become free-space radiation modes, impedance-load channels, guided port modes, or more general boundary channels. Green-function input-output relations then follow as an application, yielding frequency-dependent scattering and noise kernels without Markov or single-mode assumptions. To illustrate the practical application, we consider a lossy structure with mixed impedance and outgoing boundaries, and photonic integrated circuit configurations with waveguide port boundaries.
Abstract:We formulate a quantization scheme for open electromagnetic systems with arbitrary passive boundary conditions. Rather than specifying reservoirs phenomenologically, the method identifies them from the dissipation geometry of the Maxwell operator. Factoring the imaginary part of the Maxwell operator gives a bosonic realization of the field operator and separates the fluctuation channels into medium-assisted reservoirs from material absorption and boundary-assisted reservoirs from exchange through the open boundary. Depending on the boundary condition, the latter become free-space radiation modes, impedance-load channels, guided port modes, or more general boundary channels. Green-function input-output relations then follow as an application, yielding frequency-dependent scattering and noise kernels without Markov or single-mode assumptions. To illustrate the practical application, we consider a lossy structure with mixed impedance and outgoing boundaries, and photonic integrated circuit configurations with waveguide port boundaries.
arXiv:2606.08557 [quant-ph]
(or arXiv:2606.08557v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2606.08557 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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