Nanophotonic Quantum Processor With Nonlinear Waveguide Phase Matching

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Challenges exist in generating, manipulating, and measuring quantum states in photonic systems with the performance required for scalable quantum information systems, particularly in terms of scalability, room-temperature logical operations, and ease of encoding quantum information in both discrete and continuous variables.

Innovation Solution

A photonic integrated circuit with waveguides having second-order non-linearity is designed to operate on optical pulses with specific dimensions and engineering for phase matching and dispersion, enabling the generation, manipulation, and measurement of quantum states, including Gaussian and non-Gaussian states, using optical parametric amplifiers and oscillators.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional photonic systems are used for quantum state generation and manipulation, then room-temperature operation and scalability are achieved, but performance and efficiency are insufficient

Engineering Contradiction:
Improvequantum state generation performanceVSAvoidquantum operation efficiency
Core Design Contradiction:
ReliabilityVSProductivity

Solution Approach 1:

The patent changes the physical parameters of the photonic system by introducing waveguides with engineered second-order nonlinearity and specific dispersion characteristics. The waveguides are designed with particular geometric parameters (width, height, length) and material composition to achieve enhanced nonlinear optical interactions, thereby improving quantum state generation performance while maintaining room-temperature operation

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent applies local quality by creating regions with concentrated nonlinear optical properties within the waveguide structure. The second-order nonlinear susceptibility is localized to specific waveguide sections where quantum parametric processes occur, allowing high-efficiency quantum operations in targeted regions while other parts of the system maintain standard photonic functions

Inventive Principle:
Principle #3Local quality

2Productivity

If waveguide dimensions are reduced to enhance nonlinear efficiency, then quantum state generation efficiency improves, but tolerance to loss and fabrication precision requirements worsen

Engineering Contradiction:
Improvenonlinear interaction efficiencyVSAvoidwaveguide dimension precision
Core Design Contradiction:
ProductivityVSManufacturing precision

Solution Approach 1:

The patent employs composite waveguide structures combining multiple materials with complementary properties. The waveguides integrate materials with high nonlinear susceptibility and favorable dispersion characteristics, creating a composite structure that achieves high nonlinear efficiency without requiring extreme dimensional reductions that would demand excessive fabrication precision

Inventive Principle:
Principle #40Composite materials

Solution Approach 2:

The patent introduces dynamic tuning capabilities through phase-matching conditions that can be adjusted during operation. By controlling pump pulse parameters and waveguide phase-matching conditions, the system can optimize nonlinear interactions dynamically, compensating for variations in waveguide dimensions caused by fabrication tolerances

Inventive Principle:
Principle #15Dynamics

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The circuit achieves high nonlinear efficiency and tolerance to loss, allowing for robust quantum state generation, manipulation, and measurement, suitable for quantum computations, sensing, and error correction, with applications in quantum teleportation and boson sampling.

Implementation Method 1

one or more waveguides comprising a second order non-linearity configured to operate on classical and/or quantum optical pulses

Methodology Applied
Scientific EffectSecond-order nonlinearity:

Implementation Method 2

the one or more waveguides comprise an optical parametric amplifier and/or the circuit comprises an optical parametric oscillator comprising one of the waveguides, and the OPAs or OPOs generate the quantum states comprising signal and/or idler pulses in response to a pump pulse using a second order parametric process

Methodology Applied
Scientific EffectOptical parametric amplification:

Implementation Method 3

the pump pulses, signal pulses, and/or idler pulses each comprise an electromagnetic wave confined in and waveguided by the waveguides

Methodology Applied
Scientific EffectWaveguiding: Waveguide (optics)

Implementation Method 4

the waveguides each have dimensions including the height, the width, and the length minimizing group velocity mismatch (GVM) between the pump and signal pulses and/or idler pulses so as to provide temporal overlap of the pump and signal pulses and/or idler pulses

Methodology Applied
Scientific EffectGroup velocity matching:

Implementation Method 5

the waveguides have a phase matching and/or dispersion engineering for nonlinear interactions of the optical pulses having a bandwidth in a range of 0.1-100 Terahertz

Methodology Applied
Scientific EffectPhase matching:

Implementation Method 6

the waveguides have a phase matching and/or dispersion engineering for nonlinear interactions of the optical pulses

Methodology Applied
Scientific EffectDispersion engineering:

Data Source

PatentUS12541701B2Nanophotonic parametric quantum information processor
Publication Date: 2026.02.03 CALIFORNIA INST OF TECH
  • US12541701B2 patent drawing
  • US12541701B2 patent drawing
  • US12541701B2 patent drawing

AI summary

A photonic integrated circuit comprising one or more waveguides comprising a second order non-linearity configured to operate on optical pulses each having a pulse length shorter than 1000 optical cycles, as measured at their full width at half maximum. The circuit is configured to generate one or more quantum states carried by one or more of the optical pulses, manipulate one or more of the quantum states, and/or measure one or more of the quantum states.