Semiconductor Laser Phase Segment for Stable Single-Mode Emission

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Solution Overview

Problem

Existing methods for producing semiconductor lasers struggle to achieve reliable and replicable true single mode operation with the desired wavelength, resulting in a significant portion of scrap lasers due to imprecise mode selection and frequency fluctuations.

Innovation Solution

A method for producing semiconductor lasers that involves applying a multilayer structure on a semiconductor substrate, forming a waveguide ridge, and generating an optical element to control the phasing of amplified laser modes. The optical element is positioned at a precise distance from the lateral structure layer, ensuring that only one laser mode is amplified, thereby achieving reliable single mode operation.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Adaptability or versatility

If a periodic grating structure is used to select laser modes, then mode selection capability is improved, but manufacturing precision and reliability of single mode operation deteriorate

Engineering Contradiction:
Improvemode selection capabilityVSAvoidsingle mode operation reliability
Core Design Contradiction:
Adaptability or versatilityVSManufacturing precision

Solution Approach 1:

The laser cavity is segmented into distinct functional zones: a wavelength-selective element (grating) for mode selection and a separate optical element (phase segment) for phase control. This segmentation allows each element to perform its specific function optimally without interference, resolving the contradiction between mode selection capability and single mode operation reliability.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The phase segment acts as an intermediary element between the wavelength-selective grating and the laser gain medium. It mediates the phase relationship of amplified modes, ensuring that only the desired single mode achieves constructive interference and sustained oscillation, thereby improving manufacturing precision and reliability of single mode operation.

Inventive Principle:
Principle #24Intermediary (Mediator)

2Adaptability or versatility

If lateral structures are added for refractive index modulation, then mode selection is improved, but device complexity increases

Engineering Contradiction:
Improvemode selectionVSAvoidstructure complexity
Core Design Contradiction:
Adaptability or versatilityVSDevice complexity

Solution Approach 1:

The phase segment is merged with the waveguide ridge structure, integrating phase control functionality into the existing waveguide geometry. This merging approach adds phase control capability without requiring completely separate structural elements, thereby limiting the increase in device complexity while maintaining improved mode selection.

Inventive Principle:
Principle #5Merging (Combining)

3Measurement precision

If precise distance control is implemented for the optical element, then phasing control is improved, but manufacturing precision requirements increase

Engineering Contradiction:
Improvephasing control accuracyVSAvoiddistance tolerance
Core Design Contradiction:
Measurement precisionVSManufacturing precision

Solution Approach 1:

The phase segment is positioned at a predetermined distance from the wavelength-selective element during the fabrication process. This preliminary positioning establishes the correct phase relationship before the laser is fully assembled and tested, allowing for controlled phasing accuracy while managing manufacturing tolerance requirements through careful design of the predetermined distance.

Inventive Principle:
Principle #10Preliminary action

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 proposed method allows for the predictable and reliable production of true single mode semiconductor lasers by precisely controlling the phasing of laser modes, reducing frequency fluctuations, and minimizing scrap production.

Implementation Method 1

generating an optical element for defining the phasing of the amplified or amplifiable laser modes, the optical element being generated in such a manner that the distance in the longitudinal direction of the waveguide ridge is set such that the phasing between the lateral structure and the optical element can be controlled better than π/4

Methodology Applied
Scientific EffectPhasing control:

Implementation Method 2

The basic functional principle of the semiconductor lasers is the principle of stimulated emission. In this principle, the light of a mode or an oscillation mode is amplified exponentially when located in the amplification spectrum of the laser medium and the losses are minimized

Methodology Applied
Scientific EffectStimulated emission:

Implementation Method 3

The grating material is chosen such that a variation of the refractive index in the surroundings of the grating rods is generated in order to determine a periodic modulation of the effective complex refractive index. The periodic modulation of the refractive index leads to a strong wavelength dependence of losses or absorption

Methodology Applied
Scientific EffectPeriodic modulation of refractive index:

Data Source

PatentUS12308610B2Single mode semiconductor laser with phase control
Publication Date: 2025.05.20 ADVANCED PHOTONICS APPL GMBH
  • US12308610B2 patent drawing
  • US12308610B2 patent drawing

AI summary

The invention relates to a method for producing a semiconductor laser comprising the method steps: generating a lateral structure layer, at least in the material abrasion areas, a basic selection of the laser modes amplified or amplifiable through stimulated emission taking place via the lateral structure layer; and generating an optical element for defining the phasing of the amplified or amplifiable laser modes, the optical element being generated in such a manner that it has a distance d to an end of the lateral structure layer in the longitudinal direction of the waveguide ridge, distance d fulfilling the conditionmin⁢d-m·λe⁢f⁢f2≤λe⁢f⁢f4,m being a natural number (m∈) and λeff being the effective wavelength in the material.