Photonic Crystal Surface-Emitting Laser Optical Path Tuning

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Solution Overview

Problem

Existing methods struggle to manufacture photonic-crystal surface-emitting lasers with high accuracy in controlling oscillation wavelength and emission light characteristics due to difficulties in precisely controlling the optical path length between the photonic crystal layer and the reflection surface, leading to variations in slope efficiency and yield.

Innovation Solution

A method involving crystal growth, spectrometry, and formation of a translucent electrode with a calculated thickness to control interference between direct and reflected diffracted light, ensuring optimal light intensity conditions.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Manufacturing precision

If the optical path length is controlled by growing the semiconductor layer with high accuracy, then the oscillation wavelength and emission light characteristics can be controlled, but it is very difficult to achieve the required precision in layer thickness growth

Engineering Contradiction:
Improvelayer thickness control precisionVSAvoiddifficulty of crystal growth control
Core Design Contradiction:
Manufacturing precisionVSEase of manufacture

Solution Approach 1:

The patent applies preliminary action by forming the translucent electrode with a specific thickness range (50-200 nm) before final assembly, which preliminarily establishes the optical path length condition. This preliminary structure allows subsequent adjustment and ensures that the interference condition between direct and reflected diffracted light is satisfied, making the final optical path control more achievable.

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The patent changes the parameter approach from directly controlling semiconductor layer thickness (which is difficult) to controlling the translucent electrode thickness (which is more controllable). By adjusting the electrode thickness within 50-200 nm, the optical path length is controlled indirectly, transforming a difficult control parameter into a more manageable one while achieving the same optical interference effect.

Inventive Principle:
Principle #35Parameter changes

2Productivity

If the layer thickness is not precisely controlled, then manufacturing is easier, but the slope efficiency and emission light characteristics vary significantly

Engineering Contradiction:
Improvemanufacturing efficiencyVSAvoidconsistency of emission characteristics
Core Design Contradiction:
ProductivityVSReliability

Solution Approach 1:

The patent changes the critical parameter from semiconductor layer thickness to translucent electrode thickness. The electrode thickness can be more precisely controlled within 50-200 nm using standard deposition techniques, ensuring consistent optical interference conditions and reliable emission characteristics without sacrificing manufacturing efficiency.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The translucent electrode serves as an intermediary element that mediates between the semiconductor layer and the external environment. By controlling this intermediary layer's thickness, the patent achieves precise optical path length control and consistent emission characteristics while maintaining ease of manufacture, as the electrode can be deposited with high precision using conventional techniques.

Inventive Principle:
Principle #24Intermediary (Mediator)

3Reliability

If a reflection surface is added to improve light extraction, then emission characteristics improve, but the interference between direct and reflected diffracted light becomes difficult to control

Engineering Contradiction:
Improveemission light characteristicsVSAvoidoptical path control complexity
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The patent changes the control parameter from the complex optical path through multiple semiconductor layers to the simpler electrode thickness parameter. By controlling the electrode thickness within 50-200 nm, the interference condition is satisfied in a more straightforward manner, reducing the complexity of optical path control while maintaining reliable emission characteristics.

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

Achieves high-performance emission light characteristics with high slope efficiency and improved yield by accurately controlling the optical path length through precise layer thickness determination.

Implementation Method 1

light oscillated due to two-dimensional in-plane resonance in a photonic crystal layer is diffracted in a direction perpendicular to the plane

Methodology Applied
Scientific EffectDiffraction: Diffraction

Implementation Method 2

light diffracted in an opposite direction and reflected by a reflection surface

Methodology Applied
Scientific EffectReflection: Reflection

Implementation Method 3

light diffracted from the photonic crystal layer toward the substrate side (direct diffracted light) and light diffracted in an opposite direction and reflected by a reflection surface (reflected diffracted light) interfere with each other

Methodology Applied
Scientific EffectInterference: Interference

Data Source

PatentEP4283804B1Method of manufacturing a photonic crystal surface-emitting laser element
Publication Date: 2026.01.28 STANLEY ELECTRIC CO LTD
  • EP4283804B1 patent drawingFigure 1A
  • EP4283804B1 patent drawingFigure 1B
  • EP4283804B1 patent drawingFigure 2A

AI summary

A method of manufacturing a surface-emitting laser, includes (a) forming a first semiconductor layer including a photonic-crystal (PC) layer, (b) growing, on the first semiconductor layer, an active layer and a second semiconductor layer, (c) performing spectrometry in which a thickness from a surface of the second semiconductor layer to a position where the spectrometry light is reflected by the PC layer is measured, (d) forming a translucent electrode having a thickness calculated based on an optical path length corresponding to the thickness obtained by the spectrometry on the second semiconductor layer, and (e) forming a reflection layer on the translucent electrode, in which the layer thickness of the translucent electrode is determined such that a light intensity of interference light of (i) direct diffracted light radiated from the PC layer and (ii) reflected diffracted light radiated from the PC layer and reflected by the reflection layer is larger than a light intensity of the direct diffracted light.