Optical Devices Based on Limit Cycles and Amplification in Semiconductor Optical Cavities

Ryan Hamerly and Hideo Mabuchi
Phys. Rev. Applied 4, 024016 – Published 25 August 2015

Abstract

At strong pump powers, a semiconductor optical cavity passes through a Hopf bifurcation and undergoes self-oscillation. We simulate this device using semiclassical Langevin equations and assess the effect of quantum fluctuations on the dynamics. Below threshold, the cavity acts as a phase-insensitive linear amplifier, with noise approximately 5×larger than the Caves bound. Above threshold, the limit cycle acts as an analog memory, and the phase diffusion is approximately 10×larger than the bound set by the standard quantum limit. We also simulate entrainment of this oscillator and propose an optical Ising machine and classical controlled not (cnot) gate based on the effect.

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  • Received 16 April 2015

DOI:https://doi.org/10.1103/PhysRevApplied.4.024016

© 2015 American Physical Society

Authors & Affiliations

Ryan Hamerly* and Hideo Mabuchi

  • Edward L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA

  • *rhamerly@stanford.edu

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Vol. 4, Iss. 2 — August 2015

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