Parity-Time Symmetric Micro-Resonator for Nonreciprocal Light Transmission

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Solution Overview

Problem

Current optical systems using parity-time symmetry have limitations in achieving nonreciprocal light transmission and coexisting coherent-perfect-absorption and lasing, primarily due to the lack of resonance structures in experiments, which restrict their ability to manipulate light propagation effectively on-chip.

Innovation Solution

The development of an optical assembly comprising a first dissipative optical system and a second optical system coupled for energy transfer, where the second system receives energy from an external source and transfers it to the first system, allowing for control of energy exchange through varying coupling strength and gain, enabling nonreciprocal light transmission by operating in a broken parity-time symmetry regime.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Adaptability or versatility

If resonance structures are incorporated into PT-symmetric optical systems, then the ability to manipulate light propagation and achieve nonreciprocal transmission is improved, but the device complexity and manufacturing difficulty increase

Engineering Contradiction:
Improvelight propagation manipulation capabilityVSAvoidsystem structural complexity
Core Design Contradiction:
Adaptability or versatilityVSDevice complexity

Solution Approach 1:

The patent implements nested micro-resonators where one resonator is placed inside another, creating a compact hierarchical structure. This nesting approach achieves complex light manipulation functions within a confined geometric space, resolving the contradiction between enhanced adaptability and increased device complexity by organizing components in a space-efficient manner

Inventive Principle:
Principle #7Nested doll (Nesting)

Solution Approach 2:

The patent transitions from planar 2D photonic circuits to three-dimensional micro-resonator structures. By utilizing the third dimension (vertical stacking and spherical/cylindrical geometries), the system achieves sophisticated light propagation control and nonreciprocal transmission without proportionally increasing lateral device footprint and manufacturing complexity

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

2Adaptability or versatility

If balanced loss and gain systems are used to achieve PT-symmetry, then unconventional optical properties are obtained, but the system requires precise control of energy balance which increases operational complexity

Engineering Contradiction:
Improveunconventional optical propertiesVSAvoidenergy balance control
Core Design Contradiction:
Adaptability or versatilityVSEase of operation

Solution Approach 1:

The patent employs passive micro-resonators with inherent high quality factors that naturally store and circulate optical energy for extended periods. This self-sustaining resonance behavior reduces the need for active energy input and simplifies the balancing of gain and loss, as the system's natural resonant properties facilitate PT-symmetric operation without complex external control mechanisms

Inventive Principle:
Principle #25Self-service

Solution Approach 2:

The patent utilizes the quality factor (Q-factor) as a key parameter to characterize and control the optical resonance behavior. By designing micro-resonators with specific Q-factors and coupling them to waveguides with controlled loss rates, the system achieves PT-symmetry through parameter optimization rather than complex active control, thereby simplifying operational requirements while maintaining unconventional optical properties

Inventive Principle:
Principle #35Parameter changes

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

This approach achieves record-low power nonlinearity-induced time-reversal-symmetry-breaking for nonreciprocal light transmission, demonstrating strong nonreciprocity and enhancing nonlinearity, with applications in advanced optical systems like CPA-lasers and photonic topological insulators.

Implementation Method 1

a second optical system coupled in energy transfer communication with the first optical system. The second optical system is configured to receive a flow of energy, continuous or non-continuous/pulse, from an external source and to transfer energy to the first optical system through the coupling

Methodology Applied
Scientific EffectEnergy transfer through coupling:

Implementation Method 2

achieving record-low power nonlinearity-induced time-reversal-symmetry-breaking for nonreciprocal light transmission, demonstrating strong nonreciprocity and enhancing nonlinearity

Methodology Applied
Scientific EffectParity-time symmetry breaking:

Implementation Method 3

a first dissipative optical system... where the energy received by the second optical system is approximately equal to the energy dissipated in the first optical system

Methodology Applied
Scientific EffectOptical dissipation: Absorption (EM radiation)

Data Source

PatentUS9531150B2Method and system for parity-time symmetric optics and nonreciprocal light transmission
Publication Date: 2016.12.27 WASHINGTON UNIV IN SAINT LOUIS
  • US9531150B2 patent drawing
  • US9531150B2 patent drawing
  • US9531150B2 patent drawing

AI summary

A method and system for optical systems based on parity-time symmetry and its breaking, and for nonreciprocal light transmission in a parity-time symmetric micro-resonator system are provided. The system includes an optical assembly that includes a first dissipative optical system and a second optical system coupled in energy transfer communication with the first optical system. The second optical system is configured to receive a continuous flow of energy from an external source and to transfer energy to the first optical system through the couple wherein the energy transferred to the first optical system from the second optical system is approximately equal to the energy dissipated in the first optical system, where the energy transferred to the first optical system from the second optical system is selectable using at least one of an amount of couple between the first optical system and the second optical system and a gain of the second optical system.