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
Engineering 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
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.
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
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.
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.
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
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.
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.
Implementation Method 2
Although the waveguide and surrounding medium are configured for total internal reflection (TIR) of the probe light
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
Data Source
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.


