Curved Semiconductor Waveguide Sensor for Compact Trace Gas Detection

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Solution Overview

Problem

Existing optical absorption methods for trace gas detection in the atmosphere face limitations due to short path lengths, requiring large and expensive equipment like cavity ring-down spectrometers, and lack of sensitivity in ambient conditions.

Innovation Solution

A compact optical sensor using a curved and elongate semiconductor waveguide on a dielectric layer with integrated in-coupling and out-coupling windows, allowing for long path lengths and high sensitivity through evanescent wave interaction with analytes, utilizing materials like silicon or silicon nitride for infrared absorption.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If a straight waveguide is used, then the device occupies minimal area, but the path length is insufficient for sensitive trace gas detection

Engineering Contradiction:
Improveanalyte detection sensitivityVSAvoidwaveguide path length
Core Design Contradiction:
Measurement precisionVSLength of moving object

Solution Approach 1:

The waveguide is configured as a curved path rather than a straight line, allowing the light to traverse a much longer distance within a compact area. The curved geometry enables the probe light to interact with the analyte-containing medium over an extended path length L, directly addressing the sensitivity limitation imposed by the Beer-Lambert Law without requiring a proportionally larger device area.

Inventive Principle:
Principle #14Spheroidality (Curvature)

2Measurement precision

If cavity ring-down spectroscopy is used to achieve long path lengths, then analyte detection sensitivity is improved, but device size and cost increase significantly

Engineering Contradiction:
Improvetrace gas detection sensitivityVSAvoidsystem size and cost
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent replaces the complex mechanical cavity ring-down system with an integrated photonic waveguide structure. Instead of using mirrors spaced meters apart to achieve long path lengths, the invention uses a compact curved waveguide that confines light in an evanescent field, enabling long interaction paths within a miniaturized footprint suitable for portable applications.

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

Solution Approach 2:

The waveguide structure embeds the sensing function within a compact planar geometry. The curved waveguide path is nested within a small device footprint, allowing the light to fold back on itself multiple times through the analyte medium, achieving long effective path lengths while maintaining a small overall device size.

Inventive Principle:
Principle #7Nested doll (Nesting)

3Strength

If the waveguide is fully enclosed in dielectric material, then structural support is improved, but optical losses increase due to evanescent field interaction with the dielectric

Engineering Contradiction:
Improvestructural supportVSAvoidoptical losses
Core Design Contradiction:
StrengthVSLoss of energy

Solution Approach 1:

The dielectric layer is selectively present only in regions where structural support is needed, while the sensing region of the waveguide is left exposed to the analyte medium. This local differentiation allows the structure to maintain mechanical integrity where required while minimizing optical losses in the sensing zone by reducing evanescent field interaction with the dielectric material.

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

The sensor achieves high sensitivity and compact form factor for trace gas detection, reducing costs and complexity by integrating windows to maintain low optical losses and enabling detection without active temperature control.

Implementation Method 1

Although the waveguide and surrounding medium are configured for total internal reflection (TIR) of the probe light, analyte molecules in proximity to the waveguide are excited by the evanescent wave propagating along the exterior of the waveguide.

Methodology Applied
Scientific EffectEvanescent wave: Optical Fibre

Implementation Method 2

Although the waveguide and surrounding medium are configured for total internal reflection (TIR) of the probe light

Methodology Applied
Scientific EffectTotal internal reflection: Total Internal Reflection

Implementation Method 3

the sensitivity of analyte detection depends on the path length L over which the probe light interacts with the analyte-containing medium. This limitation comes from the familiar Beer-Lambert Law, where I is the intensity of the probe light after the interaction, I0 is the intensity before the interaction

Methodology Applied
Scientific EffectBeer-Lambert Law: Absorption Spectroscopy

Data Source

PatentUS20260063556A1Analyte sensing in a fluid medium
Publication Date: 2026.03.05 MICROSOFT TECHNOLOGY LICENSING LLC
  • US20260063556A1 patent drawing
  • US20260063556A1 patent drawing
  • US20260063556A1 patent drawing

AI summary

A method for fabricating a sensor comprises: (a) providing a wafer comprising a substrate, a dielectric layer on the substrate, and a semiconductor adlayer on the dielectric layer; (b) enacting microlithographic processing on the semiconductor adlayer to define: (i) a curved and elongate semiconductor waveguide confined to the dielectric layer, (ii) an in-coupling window arranged at a first end of the waveguide and configured to couple optically to an optical source, and (iii) an out-coupling window arranged at a second end of the waveguide and configured to couple optically to an optical detector; and (c) selectively etching the dielectric layer to define: (iv) a first dielectric region that supports and encloses the first end of the waveguide; (v) a second dielectric region that supports and encloses the second end of the waveguide; and (vi) a third dielectric region that supports but does not enclose a middle segment of the waveguide.