Type-I Interband Cascade Laser Strain Engineering

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Solution Overview

Problem

Conventional type-I mid-IR quantum well (QW) lasers face limitations in optical gain and efficiency due to the use of lattice-matched quinary AlGaInAsSb materials in barrier layers, which are difficult to calibrate and result in reduced performance compared to type-II IC lasers.

Innovation Solution

The development of type-I IC lasers with tensile strained semiconductor materials in barrier layers flanking the active region, replacing lattice-matched quinary materials, and incorporating compressive strain in the QW active region, along with tensile strained quantum wells in injectors, to enhance optical gain and reduce threshold carrier concentration.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Ease of manufacture

If lattice-matched quinary AlGaInAsSb materials are used in barrier layers, then manufacturing compatibility is improved, but optical gain is reduced and calibration difficulty increases

Engineering Contradiction:
Improvemanufacturing compatibilityVSAvoidoptical gain
Core Design Contradiction:
Ease of manufactureVSReliability

Solution Approach 1:

The patent changes the material parameters by introducing tensile strain in barrier layers and compressive strain in active regions, replacing the conventional lattice-matched quinary materials. This parameter change enables improved optical gain while maintaining manufacturability through established strain-compensated material systems.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent employs composite material structures with alternating tensile-strained barrier layers and compressive-strained active regions. This composite approach allows each layer to be optimized independently for its specific function while maintaining overall structural integrity and manufacturability.

Inventive Principle:
Principle #40Composite materials

2Reliability

If type-I QW active regions are used, then optical gain is enhanced, but free-carrier absorption loss and Auger recombination increase

Engineering Contradiction:
Improveoptical gainVSAvoidfree-carrier absorption loss
Core Design Contradiction:
ReliabilityVSLoss of energy

Solution Approach 1:

The patent applies local quality by creating distinct strain conditions in different regions: tensile strain in barrier layers to confine carriers effectively, and compressive strain in active regions to optimize optical gain. This localized strain engineering reduces free-carrier absorption loss while maintaining high optical gain in the active region.

Inventive Principle:
Principle #3Local quality

3Loss of energy

If type-II QW active regions are used, then free-carrier absorption loss is reduced, but optical gain becomes weak

Engineering Contradiction:
Improvefree-carrier absorption lossVSAvoidoptical gain
Core Design Contradiction:
Loss of energyVSReliability

Solution Approach 1:

The patent inverts the conventional type-II heterostructure approach by using type-I QW active regions with strain compensation. Instead of accepting weak optical gain from type-II structures, it uses type-I structures with optimized strain conditions to achieve both low free-carrier absorption loss and high optical gain simultaneously.

Inventive Principle:
Principle #13The other way round (Inversion)

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 configuration leads to improved output power, reduced threshold current density, and extended operational temperature range for continuous wave (cw) and pulsed lasing, enabling efficient mid-IR laser operation without the calibration challenges of quinary materials.

Implementation Method 1

The active regions of these IC lasers (referred to herein as 'type-II IC lasers') are made of type-II quantum wells (QWs) where electrons and holes are mainly distributed in separate layers

Methodology Applied
Scientific EffectQuantum confinement: Potential Well

Implementation Method 2

the wave-function overlap between the electron and hole states is relatively small. Consequently, optical gain in the type-II QW is relatively weak

Methodology Applied
Scientific EffectWave-function overlap:

Implementation Method 3

The development of type-I IC lasers with tensile strained semiconductor materials in barrier layers flanking the active region, replacing lattice-matched quinary materials, and incorporating compressive strain in the QW active region

Methodology Applied
Scientific EffectStrain engineering: Deformation

Implementation Method 4

Efficient mid-infrared (mid-IR) semiconductor lasers are needed to meet the growing demands of many civilian and military applications

Methodology Applied
Scientific EffectStimulated emission: Laser

Implementation Method 5

interband cascade (IC) lasers have been advanced to operate in continuous wave (cw) mode at room temperature (RT) and through a wide mid-IR wavelength range from 2.8 μm to 6 μm

Methodology Applied
Scientific EffectInterband transition:

Data Source

PatentUS10033160B2Interband cascade light emitting devices
Publication Date: 2018.07.24 THE BOARD OF RGT UNIV OF OKLAHOMA
  • US10033160B2 patent drawing
  • US10033160B2 patent drawing
  • US10033160B2 patent drawing

AI summary

An interband cascade (IC) light emitting device comprising a plurality of interband cascade stages, wherein at least one of the IC stages is constructed to have an electron injector made of one or more QWs, a type-I quantum well (QW) active region, a barrier layer positioned between the active region and the electron injector, a hole injector made of one or more QWs, and a barrier layer positioned between the active region and the hole injector. In at least one embodiment, a type II heterointerface layer is between the electron injector and an adjacent hole injector. The well layer of the type-I QW active region has compressive strain, while the barrier layers which flank the type-I QW active region comprise tensile strain layers. In certain embodiments, the electron injector and the hole injector comprise tensile strained layers.