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On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
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On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
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On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface

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On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface
Journal Article

On-Chip Optical Adder and Differential-Equation-Solver Based on Fourier Optics and Metasurface

2022
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Overview
Analog optical computing (AOC) has attracted great attention over the past few years, because of its ultra-high speed (potential for real-time processing), ultra-low power consumption, and parallel processing capabilities. In this article, we design an adder and an ordinary differential equation solver (ODE) on chip by Fourier optics and metasurface techniques. The device uses the 4f system consisting of two metalenses on both sides and one middle metasurface (MMS) as the basic structure. The MMS that performs the computing is the core of the device and can be designed for different applications, i.e., the adder and ODE solver in this article. For the adder, through the comparison of the two input and output signals, the effect of the addition can be clearly displayed. For the ODE solver, as a proof-of-concept demonstration, a representative optical signal is well integrated into the desired output distribution. The simulation result fits well with the theoretical expectation, and the similarity coefficient is 98.28%. This solution has the potential to realize more complex and high-speed artificial intelligence computing. Meanwhile, based on the direct-binary-search (DBS) algorithm, we design a signal generator that can achieve power splitting with the phase difference of π between the two output waveguides. The signal generator with the insertion loss of −1.43 dB has an ultra-compact footprint of 3.6 μm× 3.6 μm. It can generate a kind of input signal for experimental verification to replace the hundreds of micrometers of signal generator composed of a multi-mode interference (MMI) combination used in the verification of this type of device in the past.