Quantum Cascade Laser Layer Thickness Optimization

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Solution Overview

Problem

Conventional quantum cascade lasers face a trade-off where the reduction in transition probability from the upper energy level to the lower energy level without luminescence also decreases the luminescence transition probability, leading to decreased gain and increased threshold current.

Innovation Solution

The quantum cascade laser design includes a specific arrangement of active and injection layers with varying film thicknesses and strain levels, optimizing the band structure to increase the transition probability with luminescence while suppressing non-luminescent transitions, using AlInAs barrier layers and GaInAs quantum well layers, and adjusting the film thickness of the second barrier layer to achieve symmetry in wave functions.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Object-generated harmful factors

If the transition probability from the upper energy level to the lower energy level without luminescence is reduced, then non-luminescent transitions are suppressed, but the luminescence transition probability also decreases

Engineering Contradiction:
Improvenon-luminescent transitionsVSAvoidluminescence transition probability
Core Design Contradiction:
Object-generated harmful factorsVSReliability

Solution Approach 1:

The patent applies local quality by creating different quantum well layer thicknesses within the active layer (first quantum well layer: 1.0-3.0 nm, second quantum well layer: 3.0-6.0 nm, third quantum well layer: 3.0-6.0 nm). This local variation in thickness optimizes the wave function distribution specifically at the interface between the first quantum well layer and the second barrier layer, enhancing luminescence transition probability while suppressing non-luminescent transitions in specific regions without compromising overall laser performance.

Inventive Principle:
Principle #3Local quality

2Reliability

If the film thickness of the second barrier layer is reduced to 1.2 nm or less, then wave function symmetry is improved and luminescence transition probability increases, but manufacturing precision requirements increase

Engineering Contradiction:
Improveluminescence transition probabilityVSAvoidfilm thickness control
Core Design Contradiction:
ReliabilityVSManufacturing precision

Solution Approach 1:

The patent applies parameter changes by precisely controlling the film thickness of the second barrier layer to 1.2 nm or less (specifically 0.5-1.2 nm), which fundamentally changes the wave function distribution and symmetry. This parameter optimization creates a specific quantum confinement effect that enhances luminescence transition probability while maintaining manufacturing feasibility through established thin film deposition techniques.

Inventive Principle:
Principle #35Parameter changes

3Reliability

If the active layer structure is optimized to increase gain, then the amplification factor increases, but the device complexity increases

Engineering Contradiction:
ImprovegainVSAvoidactive layer structure
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The patent applies segmentation by dividing the active layer into three distinct quantum well layers (first: 1.0-3.0 nm, second: 3.0-6.0 nm, third: 3.0-6.0 nm) separated by barrier layers. This segmentation allows independent optimization of each layer's thickness to control electron wave function distribution, achieving high gain through enhanced luminescence transitions while maintaining a systematic and manufacturable structure.

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 design enhances the overall gain of the quantum cascade laser while maintaining a low threshold current by increasing the transition probability with luminescence and suppressing non-luminescent transitions, resulting in a higher amplification factor for light per unit length.

Implementation Method 1

An electric field is applied to this quantum cascade laser in a direction D11 indicated by an arrow in Figure 4, to inject electrons into the active layer by resonant tunneling.

Methodology Applied
Scientific EffectResonant tunneling:

Implementation Method 2

the electrons are quickly relaxed from the lower energy level to the ground energy level (relaxation energy level) by LO phonon scattering to migrate into the injection layer

Methodology Applied
Scientific EffectLO phonon scattering:

Data Source

PatentEP2498351B1Quantum cascade laser
Publication Date: 2020.12.23 SUMITOMO ELECTRIC INDUSTRIES LTD
  • EP2498351B1 patent drawingFigure 1
  • EP2498351B1 patent drawingFigure 2
  • EP2498351B1 patent drawingFigure 3

AI summary

A quantum cascade laser includes a plurality of active layers 71, each of active layers 71 including a first barrier layer B21, a first quantum well layer W21, a second barrier layer B22, a second quantum well layer W22, a third barrier layer B23, a third quantum well layer W23, and a fourth barrier layer B24 provided in this order along a predetermined direction; a plurality of injection layers 73; and a core layer having the active layers 71 and the injection layers 73, the active layers 71 and the injection layers 73 being alternately provided along the predetermined direction to form a cascade structure. The first quantum well layer W21 has a film thickness Lw21 larger than a film thickness Lw22 of the second quantum well layer W22. The second quantum well layer W22 has the film thickness Lw22 larger than a film thickness Lw23 of the third quantum well layer W23. In addition, the second barrier layer B22 has a film thickness Lb22 smaller than a film thickness Lb23 of the third barrier layer B23. The band structure produced by this layer structure achieves increase of a transition probability of electrons with luminescence and suppression of increase of a transition probability of electrons without luminescence.