Adiabatic Tapered Waveguide Edge Coupler

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Current methods for integrating photonic integrated circuits (PICs) with optical fibers face challenges due to mode size mismatch and resulting optical losses, as the mode size in high-index-contrast waveguides is much smaller than in standard single-mode fibers, leading to inefficient mode transfer.

Innovation Solution

The use of multiple adiabatic tapers in both horizontal and vertical directions to adjust the mode size, allowing for a smooth transition from a thick waveguide to a thin slab waveguide and then to a low-index waveguide, minimizing optical losses and enabling improved fabrication tolerance.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Productivity

If the mode size in the waveguide is reduced to increase integration density, then integration density is improved, but coupling efficiency to optical fibers deteriorates due to mode size mismatch

Engineering Contradiction:
Improveintegration densityVSAvoidcoupling loss
Core Design Contradiction:
ProductivityVSLoss of energy

Solution Approach 1:

The coupling device is segmented into multiple functional regions: a thick waveguide region for high-index-contrast guidance, a thin slab waveguide region for mode expansion, and transition regions with adiabatic tapers connecting them. This segmentation allows each region to be optimized for its specific function while maintaining overall coupling efficiency.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The invention transitions from a two-dimensional waveguide cross-section to a three-dimensional structure by varying the waveguide thickness (vertical dimension) in addition to width (horizontal dimension). The thick waveguide (e.g., 220 nm) transitions to a thin slab (e.g., 50-100 nm) through adiabatic tapering, enabling mode size transformation that accommodates both high integration density and efficient fiber coupling.

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

2Device complexity

If a simple inverse taper is used to transfer optical modes, then device complexity is reduced, but mode size transformation capability is limited

Engineering Contradiction:
Improvestructure complexityVSAvoidmode size transformation
Core Design Contradiction:
Device complexityVSAdaptability or versatility

Solution Approach 1:

The coupling device is divided into distinct functional segments: an initial adiabatic taper for mode preparation, a thin slab waveguide section for mode expansion, and a final adiabatic taper for fiber coupling. Each segment performs a specific transformation function, enabling comprehensive mode size adjustment that a single inverse taper cannot achieve.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

By introducing vertical thickness variation (from thick waveguide to thin slab) in addition to horizontal width variation, the device achieves enhanced mode transformation capability. The adiabatic tapering in both dimensions allows continuous mode evolution, providing adaptability for different coupling scenarios while maintaining a relatively simple overall structure.

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

3Ease of manufacture

If a thin slab waveguide is used as the edge coupler, then fabrication complexity is reduced, but mode size remains limited

Engineering Contradiction:
Improvefabrication simplicityVSAvoidmode size control
Core Design Contradiction:
Ease of manufactureVSAdaptability or versatility

Solution Approach 1:

The thick waveguide section performs preliminary mode confinement and preparation before the light enters the thin slab waveguide. This preliminary action ensures that the mode is properly prepared for the subsequent expansion in the thin slab region, enabling better mode size control and coupling efficiency while maintaining fabrication simplicity.

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The invention utilizes vertical thickness variation (from thick waveguide to thin slab) as an additional degree of freedom for mode control. This dimensional change enables the thin slab waveguide to achieve larger mode sizes at its output face compared to a conventional two-dimensional waveguide, thereby enhancing mode size control capability without complicating the fabrication process.

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

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 low-loss optical mode transfer with improved integration density and tolerance, facilitating monolithic integration with other silicon photonic components.

Implementation Method 1

a thick waveguide comprising a first adiabatic tapering from a first location to a second location... and a thin slab waveguide comprising a second adiabatic tapering from the first location to the second location

Methodology Applied
Scientific EffectAdiabatic tapering:

Data Source

PatentEP3123218B1Edge coupling using adiabatically tapered waveguides
Publication Date: 2023.07.26 HUAWEI TECH CO LTD
  • EP3123218B1 patent drawingFigure 1
  • EP3123218B1 patent drawingFigure 2
  • EP3123218B1 patent drawingFigure 3

AI summary

An apparatus comprising a thick waveguide (104) comprising a first adiabatic tapering from a first location to a second location, wherein the first adiabatic tapering is wider at the first location than at the second location, and a thin slab waveguide (106) comprising a second adiabatic tapering from the first location to the second location, wherein the second adiabatic tapering is wider at the second location than at the first location, and a third adiabatic tapering from the second location to a third location, wherein the third adiabatic tapering is wider at the second location than at the third location, wherein at least a portion of the first adiabatic tapering is adjacent to the second adiabatic tapering, and wherein the first adiabatic tapering and the second adiabatic tapering are separated from each other by a constant gap.