Vertically Stacked Slab Waveguide SHS for Spectral Resolution
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Solution Overview
Problem
Conventional grating-based spectrometers face limitations in resolution and signal-to-noise ratio due to complex fabrication processes, alignment requirements, and reduced light gathering capability, while Fourier Transform Spectrometers have undesirable moving parts, and planar waveguide technologies struggle with alignment and resolution.
Innovation Solution
A micro-spectrometer comprising vertically stacked slab waveguide spatial heterodyne spectrometer integrated circuits with variable band-pass filters and detectors to generate and process interferograms, improving resolution and signal-to-noise ratio without the need for complex alignment or moving parts.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Measurement precision
If grating-based spectrometers reduce the width of the input aperture to achieve high resolution, then spectral resolution is improved, but light gathering capability (étendue) is reduced leading to low signal to noise ratio
Solution Approach 1:
The patent transitions from conventional 2D grating-based spectrometers to a 3D integrated photonic circuit architecture where multiple waveguide layers are stacked vertically. This vertical stacking enables high spectral resolution through precise optical path difference control in the depth dimension while maintaining large étendue through parallel processing of multiple spectral channels across different layers, thereby resolving the contradiction between resolution and light gathering capability.
Solution Approach 2:
The spectrometer is segmented into multiple independent waveguide layers, each tuned to detect unique narrow spectral regions. Each layer functions as an independent spectral channel that can be processed simultaneously, allowing the system to achieve high overall resolution by combining results from multiple segments while maintaining large total étendue through parallel light collection across all layers.
2Measurement precision
If Array Waveguide Gratings use a large number of waveguides with constant length increment to disperse the spectrum, then spectral dispersion is achieved, but alignment tolerances become demanding
Solution Approach 1:
The patent merges multiple waveguide layers into a single integrated photonic circuit structure where the relative positions and orientations of layers are fixed during fabrication. This consolidation eliminates the need for separate alignment procedures for each waveguide array, as the entire multi-layer structure is manufactured as one unit with predetermined geometric relationships, thereby achieving spectral dispersion while relaxing alignment tolerance requirements.
Solution Approach 2:
The patent replaces mechanical alignment procedures with integrated photonic circuit fabrication techniques. Instead of mechanically assembling and aligning separate waveguide arrays, the system uses semiconductor manufacturing processes to create precisely positioned waveguide layers in a single integrated structure, substituting mechanical alignment precision requirements with controllable fabrication tolerances.
3Measurement precision
If Fourier Transform Spectrometers are used to deliver high resolution levels, then spectral resolution is improved, but moving parts and bulk optics are required which are undesirable in micro-spectrometers
Solution Approach 1:
The patent replaces the mechanical moving mirror of traditional Fourier Transform Spectrometers with a static integrated photonic circuit structure. The optical path difference variation traditionally achieved by mechanical mirror displacement is instead accomplished through fixed waveguide path length differences embedded in the photonic circuit geometry, eliminating moving parts while maintaining high spectral resolution through the interferometric principle.
Solution Approach 2:
The patent merges the interferometer function with the waveguide structure itself, creating an integrated photonic circuit where the waveguides serve dual purposes as both light transmission paths and interferometric elements. This consolidation eliminates separate moving components by embedding the interference function directly into the static waveguide geometry, achieving high resolution without mechanical complexity.
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
Enhances spectral resolution and signal-to-noise ratio while simplifying the alignment process and reducing manufacturing complexity, achieving high spectral resolution with improved light gathering capability.
Implementation Method 1
each slab waveguide comprising at least one slab waveguide spatial heterodyne spectrometer (SHS) tuned to detect a unique narrow spectral region of the input light signal for visualizing and measuring differences in the phase of the input light signal within the unique narrow spectral region and for generating an interferogram
Implementation Method 2
a variable band-pass filter configured to prevent aliasing of the input light signals by removing light from outside the unique narrow spectral region of each at least one slab waveguide spatial heterodyne spectrometer (SHS)
Data Source
Figure 1A~1B
Figure 1C~1D
Figure 2
AI summary
An optical broadband micro-spectrometer containing an input optical assembly, a group of slab waveguide spatial heterodyne spectrometer (SHS) integrated circuits (ICs), a detection module and a processor for multi-line detection. The input optical assembly applies an input light signal uniformly with respect to brightness and frequency to the apertures of the waveguides and may project a pupil image onto the SHS input face and may be a scanner. Each slab waveguide spatial heterodyne spectrometer (SHS) integrated circuit (IC) contains at least one slab waveguide SHS IC. The detection module bonds directly to the slab waveguide output apertures. Each slab waveguide SHS IC may contain one or more slab waveguide SHS.