Xanadu Quantum Technologies Inc.

Nicolas Quesada

Maria Schuld

Nathan Killoran

Thomas R Bromley

Juan Miguel Arrazola

Zachary Vernon

Blair Morrison

Dylan Mahler

Matteo Menotti

Kang Tan

Reihaneh Shahrokhshahi

Filippo M Miatto

Embodiments described herein provide systems and methods for optimizing a Gaussian representation to design photonic circuits for preparing a given target quantum state. The systems and methods internally consider and optimize quantum representations (e.g., Gaussian transformations, Gaussian and non-Gaussian states). In some embodiments, the systems and methods may produce optimal Gaussian transformations or states. In some embodiments, the systems and methods extract circuit parameters from an optimal Gaussian transformation to produce quantum circuits or designs for generating the optimal states. Embodiments described herein relate to systems and methods for optimizing a Gaussian transformation for state generation.

System and method to design photonic circuits for preparing Gaussian and non-Gaussian states

An apparatus includes a plurality of processing layers coupled in series. Each processing layer in the plurality of processing layers includes a Gaussian unit configured to perform a linear transformation on an input signal including a plurality of optical modes. The Gaussian unit includes a network of interconnected beamsplitters and phase shifters and a plurality of squeezers operatively coupled to the network of interconnected beamsplitters and phase shifters. Each processing layer also includes a plurality of nonlinear gates operatively coupled to the Gaussian unit and configured to perform a nonlinear transformation on the plurality of optical modes. The apparatus also includes a controller operatively coupled to the plurality of processing layers and configured to control a setting of the plurality of processing layers.

Apparatus and methods for quantum computing and machine learning

An apparatus includes an optical medium characterized by a third-order nonlinear optical susceptibility. The apparatus also includes a pump light source in optical communication with the optical medium and configured to send a pump light beam to the optical medium. The pump light beam includes a pulsed light beam. The apparatus also includes a drive light source in optical communication with the optical medium and configured to send a drive light beam to the optical medium. The drive light beam includes a continuous wave (CW) light beam. The pump light beam and the drive light beam are configured to generate a signal light beam in a squeezed state of light via spontaneous four-wave mixing in the optical medium.

Integrated devices for squeezed light generation

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Toronto, Canada

Nicolas Quesada