Vertically Emitting Semiconductor Laser Gain Modulation for Spectral Tuning

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Solution Overview

Problem

Vertically emitting semiconductor lasers exhibit a wide spectral bandwidth and require complex, costly spectral filters like etalons or birefringent filters, which impose optical losses and are difficult to adjust mechanically for rapid wavelength tuning.

Innovation Solution

A semiconductor laser design with an asymmetric periodic gain structure inside the resonant cavity, allowing adjustable optical path lengths between the gain structure and reflectors, enabling precise phase matching and spectral filtering without mechanical filters, using actuators or refractive index variations for rapid spectral tuning.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If spectral filters like etalons or birefringent filters are used to restrict spectral bandwidth, then spectral control is improved, but optical losses increase and device complexity increases

Engineering Contradiction:
Improvespectral controlVSAvoidoptical losses
Core Design Contradiction:
Measurement precisionVSLoss of energy

Solution Approach 1:

The patent extracts and eliminates the need for separate spectral filter components (etalons, birefringent filters) by integrating spectral control functionality directly into the periodic gain structure itself. The periodic modulation of the gain medium provides inherent spectral selectivity without requiring additional optical filter elements in the cavity.

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent merges the spectral filtering function with the gain structure by periodically modulating the gain medium's properties. This combines what were previously separate functions (gain provision and spectral filtering) into a single integrated component, reducing overall device complexity and optical losses.

Inventive Principle:
Principle #5Merging (Combining)

2Measurement precision

If mechanical filters are used for wavelength tuning, then spectral control is improved, but device complexity increases and adjustment speed decreases

Engineering Contradiction:
Improvewavelength tuningVSAvoidmechanical adjustment complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent replaces mechanical filter adjustment mechanisms with direct electrical or optical control of the periodic gain structure's properties. By modulating the gain medium's periodic structure through non-mechanical means (such as electrical fields, temperature control, or optical pumping), the system achieves wavelength tuning without moving parts, thereby reducing complexity and enabling faster response times.

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

Solution Approach 2:

The patent introduces dynamic control of the periodic gain structure parameters, allowing real-time adjustment of spectral characteristics. The periodic modulation depth, frequency, or phase can be dynamically changed to tune the laser wavelength, providing fast and flexible spectral control without mechanical intervention.

Inventive Principle:
Principle #15Dynamics

3Manufacturing precision

If periodic gain structure is monolithically integrated with reflectors, then manufacturing precision is improved, but spectral bandwidth becomes too wide for many applications

Engineering Contradiction:
Improvemonolithic integrationVSAvoidspectral bandwidth control
Core Design Contradiction:
Manufacturing precisionVSMeasurement precision

Solution Approach 1:

The patent applies local quality modification by periodically modulating specific regions of the gain structure while maintaining overall monolithic integration. The periodic variation in gain properties at specific locations within the active medium provides spectral selectivity without compromising the benefits of monolithic construction. This localized periodic modulation creates wavelength-specific gain regions that narrow the spectral bandwidth while preserving manufacturing simplicity.

Inventive Principle:
Principle #3Local quality

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 precise spectral control and tunability with reduced optical losses, allowing fast and efficient adjustment of laser emission characteristics.

Implementation Method 1

the quantum wells and hence the periodic gain structure provides optical gain

Methodology Applied
Scientific EffectStimulated emission: Laser

Implementation Method 2

a first reflector and a second reflector. The second reflector is separated from the first reflector along a longitudinal direction

Methodology Applied
Scientific EffectReflection: Reflection

Implementation Method 3

the standing wave pattern of the resonator or resonant cavity

Methodology Applied
Scientific EffectInterference: Interference

Implementation Method 4

Matching of the periodic gain structure with the standing wave pattern of the intracavity laser radiation may be assured by monolithic construction

Methodology Applied
Scientific EffectPhase modulation: Phase Modulation

Data Source

PatentEP4686016A1Gain modulation of vertically emitting semiconductor lasers
Publication Date: 2026.01.28 TWENTY ONE SEMICON GMBH
  • EP4686016A1 patent drawingFigure 1~2
  • EP4686016A1 patent drawingFigure 3~5
  • EP4686016A1 patent drawingFigure 6~7

AI summary

The present disclosure relates to a semiconductor laser comprising: - a first reflector (12), - a second reflector (14) separated from the first reflector (12) along a longitudinal direction (z), - a resonant cavity (8) confined by the first reflector (12) and by the second reflector (14), - a periodic gain structure (16) inside the resonant cavity (8), the periodic gain structure (16) is separated from the first reflector (12) by a first optical path length (L1) and is separated from the second reflector (14) by a second optical path length (L2), wherein the first optical path length (L1) is shorter than the second optical path length (L2), characterized in that - the first optical path length (L1) between the periodic gain structure (16) and the first reflector (12) is adjustable.