Polarization-Splitting Optical Coupler with Resonant Directional Coupling

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Solution Overview

Problem

Existing polarization-separating optical couplers suffer from inefficiencies in separating optical modes based on polarization states, leading to high optical losses and sensitivity to wavelength variations.

Innovation Solution

A polarization separation optical coupler with two waveguides having distinct refractive index deviations and constant transverse dimensions, ensuring equal effective indices for one polarization state and unequal indices for the other, employing resonant directional coupling to enhance separation efficiency.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If adiabatic coupling is used to separate polarization states, then polarization separation is achieved, but the coupling length becomes excessively long and optical losses increase

Engineering Contradiction:
Improvepolarization separation performanceVSAvoidcoupling length
Core Design Contradiction:
ReliabilityVSLength of stationary object

Solution Approach 1:

The patent changes the refractive index parameter of the waveguide to enable resonant coupling. By setting the waveguide refractive index to match the surrounding medium (Δn = 0), the effective indices for both polarizations become equal, creating phase-matching conditions that enable efficient coupling over a short distance, thereby resolving the contradiction between separation performance and coupling length

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent employs resonant coupling by exciting specific polarization modes at their resonant frequencies. The resonant condition creates strong coupling between the waveguide mode and the surrounding medium mode, enabling efficient polarization separation in a compact structure without requiring long adiabatic taper lengths

Inventive Principle:
Principle #18Mechanical vibration

2Reliability

If adiabatic coupling is used to separate polarization states, then polarization separation is achieved, but optical losses increase

Engineering Contradiction:
Improvepolarization separation performanceVSAvoidoptical losses
Core Design Contradiction:
ReliabilityVSLoss of energy

Solution Approach 1:

By changing the refractive index parameter to match conditions (Δn = 0), the patent achieves resonant phase-matching that enables efficient coupling. This resonant condition maximizes energy transfer between modes while minimizing radiative losses, thereby achieving good polarization separation with low optical losses

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The resonant coupling mechanism excites specific polarization modes at their natural frequencies, creating constructive interference that enhances coupling efficiency. This resonant enhancement allows for low-loss polarization separation by concentrating energy transfer at specific frequencies rather than requiring gradual adiabatic transformation

Inventive Principle:
Principle #18Mechanical vibration

3Reliability

If adiabatic coupling is used to separate polarization states, then polarization separation is achieved, but the device becomes highly sensitive to wavelength variations

Engineering Contradiction:
Improvepolarization separation performanceVSAvoidwavelength sensitivity
Core Design Contradiction:
ReliabilityVSAdaptability or versatility

Solution Approach 1:

The resonant coupling mechanism creates sharp frequency-selective response that enhances polarization separation at the resonant wavelength. The resonant condition provides strong wavelength discrimination, allowing the device to maintain high separation performance while being tunable to specific wavelength bands of interest

Inventive Principle:
Principle #18Mechanical vibration

4Reliability

If different refractive index deviations are used in the two waveguides, then resonant coupling is achieved for improved separation, but manufacturing precision requirements increase

Engineering Contradiction:
Improvepolarization separation performanceVSAvoidrefractive index control precision
Core Design Contradiction:
ReliabilityVSManufacturing precision

Solution Approach 1:

The patent sets the refractive index deviation to zero (Δn = 0), which simplifies the manufacturing requirement to matching the waveguide index to the surrounding medium. This parameter choice creates a well-defined target value that can be achieved through standard fabrication processes, balancing performance requirements with manufacturing feasibility

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

The coupler achieves low optical losses and reduced wavelength sensitivity, with a significantly shorter coupling length and improved extinction ratio compared to adiabatic couplers.

Implementation Method 1

two waveguides optically coupled to each other in an evanescent manner

Methodology Applied
Scientific EffectEvanescent coupling:

Implementation Method 2

employing resonant directional coupling to enhance separation efficiency

Methodology Applied
Scientific EffectResonant directional coupling: Resonance

Data Source

PatentEP4614200A1Polarization splitting optical coupler
Publication Date: 2025.09.10 TEEM PHOTONICS
  • EP4614200A1 patent drawingFigure 1A~1B
  • EP4614200A1 patent drawingFigure 2A~2B
  • EP4614200A1 patent drawingFigure 3A~3B

AI summary

The invention relates to a polarization-separating optical coupler comprising a first waveguide (10) and a second waveguide (20) optically coupled to each other, the first waveguide (10) supporting optical modes polarized according to a first and a second distinct polarization state (P1; P2) at a wavelength λc and the second waveguide (20) supporting an optical mode polarized according to the first polarization state at the wavelength λc. The first and second waveguides (10, 20) are configured such that there is equality, over the entire length of the optical coupler (1), of the effective indices n1eff_P1 and n2eff_P1 associated with the first polarization state, resulting in an inequality of the effective indices n1eff_P2 and n2eff_P2 associated with the second polarization state.