Double Beam Interferometer for Single Shot Hyperspectral Imaging
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Solution Overview
Problem
Existing Fourier Transformation Spectrometers face challenges in achieving robust, efficient hyperspectral imaging of moving objects and turbulent scenes due to limitations in beam path stability, field of view discrimination, and signal-to-noise ratio, particularly when using unstable light sources and in environments with vibrations.
Innovation Solution
A double beam interferometer with field of view discriminators and a cyclical or non-cyclical configuration, including beam splitters and deflection units, generates lateral shear and spatially overlays partial beams to produce multiple spatial interferograms simultaneously, enabling single shot hyperspectral imaging with improved stability and signal-to-noise ratio.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If a conventional Fourier Transformation Spectrometer is used with unstable light sources, then the spectral measurement can be performed, but the signal-to-noise ratio deteriorates and measurement precision is reduced
Solution Approach 1:
The detector is divided into multiple detector fields that simultaneously record multiple spatial interferograms. Each detector field captures interferogram data for a specific spatial region, allowing parallel acquisition of spectral information from different areas of the scene. This segmentation enables the system to maintain high signal-to-noise ratio even with unstable light sources by distributing the measurement across multiple independent detection channels.
Solution Approach 2:
The patent employs a cyclical interferometer configuration where the optical path difference varies periodically, creating a cyclical pattern in the interferogram data. This periodic action allows the system to capture complete spectral information through Fourier transformation of the periodic interferogram signals, maintaining measurement precision despite light source instability.
2Productivity
If the spectrometer is used for hyperspectral imaging of moving objects, then the imaging speed is improved, but the beam path stability deteriorates due to vibrations and motion
Solution Approach 1:
The optical system is segmented into multiple independent beam paths, with each beam path directed to a separate detector field. This segmentation allows the system to capture spatial interferograms from different regions simultaneously, making the overall measurement less sensitive to vibrations and motion-induced beam path instability. Each segmented beam path acts as an independent measurement channel that can tolerate certain levels of disturbance.
Solution Approach 2:
The field of view discriminators are positioned to pre-select and define the spatial regions of interest before the light enters the interferometer. This preliminary spatial filtering ensures that only the desired field of view reaches the detector, maintaining image quality and reducing the impact of motion-induced aberrations by establishing the measurement geometry in advance.
3Measurement precision
If field of view discrimination is implemented to improve spatial resolution, then the spatial selectivity is improved, but the device complexity increases
Solution Approach 1:
The patent merges the field of view discrimination function with the interferometer's existing optical components. The field of view discriminators are integrated into the beam path without requiring separate, independent spatial filtering systems. This merging approach achieves spatial resolution improvement while minimizing additional device complexity by utilizing the interferometer's inherent optical architecture.
Solution Approach 2:
The optical components in the interferometer serve multiple functions: beam splitting, spatial filtering, and interferogram generation. The field of view discriminators not only provide spatial selection but also work in conjunction with the beam deflection units to direct light to appropriate detector fields. This multi-functionality reduces the need for additional specialized components, thereby limiting the increase in device complexity.
4Productivity
If multiple spatial interferograms are recorded simultaneously to improve imaging efficiency, then the productivity is improved, but the device complexity increases
Solution Approach 1:
The detector is segmented into multiple detector fields that can simultaneously record multiple spatial interferograms. Each detector field is assigned to capture interferogram data from a specific spatial region or wavelength range. This segmentation enables parallel acquisition of spectral information, dramatically improving imaging efficiency while keeping the detector technology itself relatively simple and well-established.
Solution Approach 2:
The patent extends the measurement from a single spatial interferogram in one dimension to multiple spatial interferograms across two or more detector fields. This dimensional extension allows simultaneous recording of spectral information from multiple spatial locations or spectral regions, improving productivity by utilizing the additional spatial or spectral dimensions provided by the multi-field detector arrangement.
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 configuration allows for robust, efficient hyperspectral imaging of moving objects and turbulent scenes with reduced errors and increased stability, enabling fast and accurate spectral analysis even under unsettled conditions.
Implementation Method 1
at least one beam splitter unit to split an incident light beam and/or an input beam of a spatially expanded object into a first partial beam and a second partial beam
Implementation Method 2
the beam splitter unit is also designed to spatially at least partially overlay the first partial beam and the second partial beam with a lateral shear
Implementation Method 3
at least one first beam deflection unit designed to deflect the first partial beam at least a first and a second time; at least one second beam deflection unit designed to deflect the second partial beam at least a first and a second time
Implementation Method 4
wherein the respectively first and second deflection of the first partial beam and the second partial beam generates the lateral shear
Implementation Method 5
at least one first field of view discriminator unit arranged in the double beam interferometer such that the first partial beam is spatially selected after the splitting and before the second deflection; at least one second field of view discriminator unit arranged in the double beam interferometer such that the second partial beam is spatially selected after the splitting and before the second deflection
Implementation Method 6
at least one lens arranged opposite the beam splitter unit such that the incident light passes the lens at least partially before said light beam is split on the beam splitter unit and the first partial beam and the second partial beam respectively generate a plurality of coherent image points of the spatially expanded object in an image plane
Implementation Method 7
the detector having at least one detector field to record a plurality of spatial interferograms on the basis of the spatial overlay of the first partial beam and the second partial beam
Implementation Method 8
at least one computing unit for the Fourier transformation of the plurality of spatial interferograms to generate a plurality of spectrums
Data Source
AI summary
Fourier Transformation Spectrometer, FT Spectrometer, comprising: A double beam interferometer, comprising: At least one beam splitter unit (622; 623; 624, 625, 626, 627; 636; 673, 674, 675) for splitting an incident light beam (EB) of a spatially expanded object into a first partial beam (TB1) and a second partial beam (TB2); at least a first beam deflection unit (630; 641; 651; 661; 697) designed to deflect the first partial beam (TB1) at least a first and a second time, wherein the second beam deflection unit (630) is designed to also deflect the second partial beam (TB2) at least at first and a second time; or the double beam interferometer comprises a second beam deflection unit (642; 652; 662) designed to deflect the second partial beam (TB2) at least a first and a second time, wherein the beam deflection unit is also designed to at least partially spatially overlay the first partial beam (TB1) and the second partial beam (TB2), and the respectively first and second deflection of the first partial beam (TB1) and of the second partial beam (TB2) generates a lateral shear (s); at least a first field of view discriminator unit (BFD1; 631; 645; 653; 656; 666; 677; 976) arranged such that the first partial beam (TB1) is spatially selected after the splitting and prior to the second deflection; at least a second field of view discriminator unit (BFD2; 632; 646; 654; 657; 667; 678; 977) arranged such that the second partial beam (TB2) is spatially selected after the splitting and prior to the second deflection.


