Abstract

Ultracompact nonlinear optical devices utilizing two-dimensional (2D) materials and nanostructures are emerging as important elements of photonic circuits. Integration of the nonlinear material into a subwavelength cavity or waveguide leads to a strong Purcell enhancement of the nonlinear processes and compensates for a small interaction volume. The generic feature of such devices which makes them especially challenging for analysis is strong dissipation of both the nonlinear polarization and highly confined modes of a subwavelength cavity. Here we solve a quantum-electrodynamic problem of the spontaneous and stimulated parametric down-conversion in a nonlinear quasi-2D waveguide or cavity. We develop a rigorous Heisenberg-Langevin approach which includes dissipation and fluctuations in the electron ensemble and in the electromagnetic field of a cavity on equal footing. Within a relatively simple model, we take into account the nonlinear coupling of the quantized cavity modes, their interaction with a dissipative reservoir and the outside world, amplification of thermal noise and zero-point fluctuations of the electromagnetic field, and other relevant effects. We derive closed-form analytic results for relevant quantities such as the spontaneous parametric signal power and the threshold for parametric instability. We find a strong reduction in the parametric instability threshold for 2D nonlinear materials in a subwavelength cavity and provide a comparison with conventional nonlinear photonic devices.

Highlights

  • INTRODUCTIONEnhancement of the radiative processes due to the localization of emitters in a subwavelength cavity (the so-called Purcell enhancement1) is a fundamental cavity quantum electrodynamics (QED) effect of great importance for numerous applications

  • Enhancement of the radiative processes due to the localization of emitters in a subwavelength cavity is a fundamental cavity quantum electrodynamics (QED) effect of great importance for numerous applications

  • The nonlinear optics has received relatively less attention; recent advancements in strong light localization using subwavelength cavities, photonic crystals, metamaterials, and metasurfaces enabled the nonlinear optics in ultrasmall volumes and at relatively low power levels; see, e.g., Refs. 2–10 and references therein

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Summary

INTRODUCTION

Enhancement of the radiative processes due to the localization of emitters in a subwavelength cavity (the so-called Purcell enhancement1) is a fundamental cavity quantum electrodynamics (QED) effect of great importance for numerous applications. The rise of two-dimensional (2D) materials with atomic monolayer thickness and excellent nonlinear optical properties, such as graphene and transition metal dichalcogenide monolayers, has enabled quasi-2D cavities and waveguides only a few nm thick.17,18 These advances create new exciting opportunities for ultracompact nonlinear optical devices and raise important issues of the correct description of quantum fields in systems with strong dissipation both in a macroscopic ensemble of fermionic emitters. One important application for Purcell-enhanced nonlinear optics is compact systems for generation of squeezed and entangled photon states as a result of parametric downconversion. It derives convenient analytic expressions for the spontaneous parametric signal, the parametric amplification threshold in plane-parallel cavities, and the signal evolution at the linear stage. Our results show that it is possible to achieve a significant reduction in the parametric amplification threshold due to Purcell enhancement in quasi-2D subwavelength cavities

PARAMETRIC DOWN-CONVERSION IN A CONSERVATIVE SYSTEM
EQUATIONS FOR PARAMETRIC DOWN-CONVERSION IN A DISSIPATIVE SYSTEM
K1 are eigenvalues and eigenvectors of the
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