Mid-Infrared Quantum Cascade Laser Waveguide for Compact Chip Coupling

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Solution Overview

Problem

Conventional photonic circuits are unable to efficiently couple quantum cascade lasers emitting in the mid-infrared range due to low refractive index contrast materials, resulting in large and cumbersome gas sensors.

Innovation Solution

A quantum cascade laser design that emits a transverse magnetic polarized optical mode using a main waveguide with a core made of Group IV A atoms and silicon nitride or chalcogenide confinement layers, integrated with a diffraction grating for distributed feedback, allowing optical coupling to compact photonic chips with high refractive index contrast.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional photonic circuits with silicon oxide layers are used, then the photonic circuit can be manufactured with standard materials, but the circuit cannot efficiently transmit mid-infrared light from quantum cascade lasers

Engineering Contradiction:
Improveoptical coupling efficiencyVSAvoidmaterial compatibility
Core Design Contradiction:
ReliabilityVSEase of manufacture

Solution Approach 1:

The patent changes the material parameters of the photonic circuit by replacing silicon oxide with silicon nitride or chalcogenide materials that have appropriate refractive indices for mid-infrared transmission. This material substitution enables efficient optical coupling with quantum cascade lasers while maintaining manufacturability through standard semiconductor fabrication processes.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent employs composite material structures in the photonic circuit, combining silicon nitride or chalcogenide confinement layers with Group IV A atom-based core materials. This composite approach optimizes both optical performance in the mid-infrared range and compatibility with existing manufacturing techniques.

Inventive Principle:
Principle #40Composite materials

2Reliability

If waveguides with low refractive index contrast are used to couple quantum cascade lasers, then optical coupling is achieved, but the waveguides become large and the photonic chip size increases

Engineering Contradiction:
Improveoptical coupling efficiencyVSAvoidphotonic chip area
Core Design Contradiction:
ReliabilityVSArea of stationary object

Solution Approach 1:

The patent changes the refractive index parameter by introducing high-refractive-index materials (silicon nitride or chalcogenide) as confinement layers. This increases the refractive index contrast between the core and confinement regions, enabling compact waveguide dimensions while maintaining efficient optical coupling with quantum cascade lasers.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent introduces an intermediary optical mode (antisymmetric supermode) that mediates the coupling between the quantum cascade laser and the photonic circuit. This supermode is supported by the specific waveguide geometry and material combination, enabling efficient energy transfer while allowing compact waveguide design.

Inventive Principle:
Principle #24Intermediary (Mediator)

3Reliability

If large waveguides with low refractive index contrast are used, then optical coupling is maintained, but the gas sensor chamber and overall sensor size become large

Engineering Contradiction:
Improveoptical coupling efficiencyVSAvoidsensor compactness
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The patent changes the optical parameters of the waveguide system by using high-refractive-index materials, which enables smaller waveguide dimensions. This reduction in waveguide size directly leads to a more compact gas sensor chamber and overall sensor design, while maintaining reliable optical coupling between the quantum cascade laser and photonic circuit.

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

Enables efficient optical coupling of quantum cascade lasers to photonic circuits, reducing sensor size and enhancing performance by maintaining a high Side Mode Suppression Ratio (SMSR) and enabling compact, high-refractive index photonic chips for gas detection applications.

Implementation Method 1

A grating satisfying the Bragg condition at the emission wavelength is structured in or on the gain medium so as to diffract the laser optical mode to make it travel back and forth within the gain medium.

Methodology Applied
Scientific EffectBragg diffraction: Bragg Diffraction

Implementation Method 2

The gain medium has geometric dimensions and refractive indices enabling the guiding of a laser optical mode at an emission wavelength along an optical axis of the gain medium.

Methodology Applied
Scientific EffectTotal internal reflection: Total Internal Reflection

Implementation Method 3

The lower and upper confinement layers each have a refractive index lower than a minimum refractive index of the active region.

Methodology Applied
Scientific EffectTotal internal reflection: Total Internal Reflection

Data Source

PatentUS20250372949A1Mid-infrared emitting quantum cascade laser
Publication Date: 2025.12.04 COMMISSARIAT A LENERGIE ATOMIQUE ET AUX ENERGIES ALTERNATIVES
  • US20250372949A1 patent drawing
  • US20250372949A1 patent drawing
  • US20250372949A1 patent drawing

AI summary

The invention relates to a quantum cascade laser emitting a TM polarized optical mode with a wavelength between 3 and 15 μm, including a gain medium and a main waveguide. The latter includes a coupling section in contact with the gain medium, comprising a DFB diffraction grating. The coupling section has a width greater than or equal to a minimum width from which an antisymmetric supermode propagating in a laser guiding structure comprising the gain medium and the main waveguide, has a confinement factor in an active region of the gain medium strictly greater than those of the optical modes likely to be guided by the guiding structure. The main waveguide includes a core based on atoms from column IV A of the periodic table of elements and a SiN or chalcogenide confinement sublayer.