Heterogeneous GaN Laser Coupling With an Intermediate Waveguide

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Solution Overview

Problem

The integration of GaN-based active devices with high-performance waveguides in photonic integrated circuits (PICs) faces challenges due to the large refractive index difference between materials, requiring precise alignment and narrow taper tips for efficient optical coupling, which is costly and limits scalability.

Innovation Solution

The use of a butt-coupling approach combined with a mode-converter intermediate waveguide facilitates efficient optical coupling between dissimilar materials, reducing the need for narrow taper tips and allowing for more relaxed taper dimension requirements, thus enabling scalable manufacturing of GaN-based PICs.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Loss of energy

If traditional tapered coupling is used to transfer optical signals between dissimilar materials with large refractive index differences, then efficient power transfer can be achieved, but the taper tip dimensions become extremely small which increases manufacturing complexity and costs

Engineering Contradiction:
Improveoptical coupling lossVSAvoidtaper fabrication complexity
Core Design Contradiction:
Loss of energyVSDevice complexity

Solution Approach 1:

The patent introduces an intermediate waveguide layer with refractive index between the high-index GaN active device and low-index dielectric waveguide. This intermediate layer acts as a mediator that gradually transitions the optical mode from the GaN waveguide to the dielectric waveguide, avoiding the need for extremely narrow taper tips while maintaining efficient coupling. The intermediate layer has refractive index approximately 2.0-2.2, positioned between GaN (>2.4) and dielectric materials (1.44-2.0).

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The patent changes the refractive index parameter by introducing an intermediate material layer with specific refractive index properties. This parameter change allows for relaxed taper dimensions while maintaining efficient optical coupling. The intermediate layer's refractive index is specifically selected to be between that of GaN and the dielectric waveguide material, enabling gradual mode transformation.

Inventive Principle:
Principle #35Parameter changes

2Loss of energy

If narrow taper tips are used to achieve efficient coupling between GaN and dielectric materials, then optical power transfer is improved, but electrical pumping becomes challenging and may result in increased coupling losses

Engineering Contradiction:
Improveoptical coupling lossVSAvoidelectrical pumping feasibility
Core Design Contradiction:
Loss of energyVSEase of manufacture

Solution Approach 1:

The intermediate waveguide layer provides a broader transition region that can be electrically pumped more effectively. Instead of concentrating the optical mode in an extremely narrow taper tip that is difficult to pump, the intermediate layer distributes the mode over a larger area, making electrical pumping feasible and reliable while still achieving efficient coupling to the final dielectric waveguide.

Inventive Principle:
Principle #24Intermediary (Mediator)

3Loss of energy

If precise alignment and narrow taper tips are required for efficient coupling, then optical coupling efficiency is improved, but packaging costs increase and scaling is limited

Engineering Contradiction:
Improveoptical coupling lossVSAvoidmanufacturing scalability
Core Design Contradiction:
Loss of energyVSProductivity

Solution Approach 1:

The intermediate waveguide layer creates a more robust coupling structure that is less sensitive to alignment errors. The gradual mode transformation through the intermediate layer provides a larger tolerance window for alignment, enabling less precise packaging processes and facilitating scaling to mass production while maintaining efficient optical coupling.

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The coupling structure is segmented into multiple stages: GaN active device, intermediate waveguide layer, and final dielectric waveguide. This segmentation allows each component to be optimized independently and assembled with relaxed alignment requirements, improving manufacturability and scalability compared to a single-stage narrow-taper approach.

Inventive Principle:
Principle #1Segmentation

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 solution achieves efficient optical coupling with reduced stringent requirements on taper tip widths, facilitating scalable manufacturing and improved performance of GaN-based PICs, including lasers, amplifiers, modulators, and photodetectors.

Implementation Method 1

a mode-converter intermediate waveguide facilitates efficient coupling between modes in the active and passive layers

Methodology Applied
Scientific EffectMode conversion:

Implementation Method 2

efficient coupling between modes in the active and passive layers is facilitated by use of a butt-coupling approach in combination with the mode-converter

Methodology Applied
Scientific EffectOptical coupling:

Data Source

PatentUS12271033B2Heterogeneous GaN lasers and active components
Publication Date: 2025.04.08 NEXUS PHOTONICS INC
  • US12271033B2 patent drawing
  • US12271033B2 patent drawing
  • US12271033B2 patent drawing

AI summary

A device comprises first, second, third and fourth elements fabricated on a common substrate. The first element comprises an active waveguide structure supporting a first optical mode, the second element comprises a passive waveguide structure supporting a second optical mode, the third element, at least partly butt-coupled to the first element, comprises an intermediate waveguide structure supporting intermediate optical modes, and a fourth element comprising TCO material that is attached to the first element. If the first optical mode differs from the second optical mode by more than a predetermined amount, a tapered waveguide structure in at least one of the second and third elements facilitates efficient adiabatic transformation. No adiabatic transformation occurs between any of the intermediate optical modes and the first optical mode. Mutual alignments of the first, the second, the third, and the fourth elements are defined using lithographic alignment marks.