Multispectral Raman Spectroscopy for Flowing Samples

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Solution Overview

Problem

Conventional Raman spectroscopy setups are inadequate for analyzing moving samples due to difficulties in tracking excitation and detection of scattered radiation, leading to impaired signal quality and inability to record complete Raman spectra within short measurement times, especially in flow cytometry applications.

Innovation Solution

An optical system with a multispectral excitation source emitting monochromatic radiation at multiple wavelengths along a common beam axis, combined with an elongate flow-through region and a detection device for wavelength-selective filtering, allows for the examination of moving sample elements by irradiating excitation radiation at multiple positions and detecting scattered radiation at different wavelengths, reducing measurement times and enabling compact, robust setups.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Productivity

If conventional Raman spectroscopy setups are used to analyze moving samples, then excitation and detection can be performed, but signal quality is impaired and complete Raman spectra cannot be recorded within short measurement times

Engineering Contradiction:
Improvemeasurement speedVSAvoidsignal quality
Core Design Contradiction:
ProductivityVSMeasurement precision

Solution Approach 1:

The system segments the spectrum detection process by using multiple detection channels, each equipped with specific filter combinations tuned to detect different spectral regions simultaneously. This allows parallel detection of multiple wavelength ranges, enabling complete spectral acquisition within the short measurement time window of flowing samples while maintaining signal quality through dedicated detection paths for each spectral region

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The invention transitions from sequential spectral scanning to simultaneous multi-wavelength detection by adding a spectral dimension to the detection process. Multiple detection channels operate in parallel at different wavelength ranges, effectively converting a time-based sequential measurement approach into a spatially parallel approach, thereby achieving both high measurement speed and complete spectral coverage

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

2Measurement precision

If stationary samples are used for Raman spectroscopy, then measurement background can be suppressed by integrating over long measurement periods, but the setup cannot track moving samples

Engineering Contradiction:
Improvebackground suppressionVSAvoidsample movement tracking
Core Design Contradiction:
Measurement precisionVSAdaptability or versatility

Solution Approach 1:

The system employs periodic modulation of the excitation light source at specific frequencies, which allows the Raman signal to be distinguished from the continuous background fluorescence through frequency-based filtering. This periodic excitation approach enables background suppression even with moving samples by locking onto the modulated signal frequency, eliminating the need for long integration periods on stationary samples

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The invention replaces the mechanical tracking system (moving mirrors or stages to follow sample position) with an optical field-based approach where the excitation and detection are configured to illuminate and collect signals from a defined measurement volume in the flow path. The system uses flow cytometry principles where samples pass through a fixed measurement zone, eliminating mechanical tracking while maintaining measurement capability on moving samples

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

3Measurement precision

If conventional spectrometers are used for continuous Raman spectrum recording, then complete spectra can be obtained, but integration and measurement times are too long for moving samples

Engineering Contradiction:
Improvespectral completenessVSAvoidmeasurement time
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The detection system is segmented into multiple parallel channels, each detecting a specific wavelength range simultaneously. This segmentation allows the complete spectrum to be reconstructed from multiple simultaneous measurements rather than sequential scanning, reducing the measurement time from seconds to microseconds while maintaining full spectral coverage

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The invention merges multiple detection channels with different filter combinations into a single integrated detection system. Each channel detects a portion of the spectrum simultaneously, and the signals are combined to form a complete Raman spectrum. This merging of parallel detection paths achieves both spectral completeness and rapid measurement times suitable for flowing samples

Inventive Principle:
Principle #5Merging (Combining)

4Productivity

If flow cytometry is used for particle analysis, then individual sample elements can be examined, but Raman spectra cannot be recorded due to short observation time

Engineering Contradiction:
Improvesample throughputVSAvoidspectral detection capability
Core Design Contradiction:
ProductivityVSMeasurement precision

Solution Approach 1:

The excitation source is modulated periodically, allowing the Raman signal to be detected through synchronous detection techniques that filter out the much stronger continuous fluorescence background. This periodic excitation enables Raman spectroscopy in the flow cytometry context by creating a time-resolved signal that can be extracted from the rapid flow environment

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The detection system is divided into multiple channels with specific filter sets optimized for different spectral regions, allowing simultaneous detection of multiple Raman lines. This segmentation enables complete spectral acquisition during the brief observation time of flowing particles by capturing different spectral components in parallel rather than sequentially

Inventive Principle:
Principle #1Segmentation

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 approach enables rapid recording of Raman spectra from moving samples without complex setups, using inexpensive components, and provides precise intensity measurements of Raman lines, overcoming the limitations of conventional Raman spectroscopy in flow cytometry and other applications.

Implementation Method 1

a laser device that can be switched on and off between at least two different wavelengths and that emits along a common beam axis

Methodology Applied
Scientific EffectLight emission from laser source: Laser

Implementation Method 2

inelastically scattered by the sample. The scattered excitation radiation can then be collected using a suitable spectroscopy arrangement and examined spectrally

Methodology Applied
Scientific EffectRaman scattering: Scattering

Implementation Method 3

a detection device for wavelength-selective filtering and detection of at least part of the scattered radiation

Methodology Applied
Scientific EffectWavelength-selective filtering: Filter (optical)

Data Source

PatentEP3309538B1Optical system and method for spectroscopy
Publication Date: 2022.02.16 FERDINAND BRAUN INSTITUT GGMBH LEIBNIZ INSTITUT FUR HOCHSTFREQUENZTECHNIK
  • EP3309538B1 patent drawingFigure 1A
  • EP3309538B1 patent drawingFigure 1B~1C
  • EP3309538B1 patent drawingFigure 2

AI summary

The invention relates to an optical system and a method for spectroscopy. The optical system (100) according to the invention is particularly suitable for Raman spectroscopy and comprises a multispectral excitation source (10) configured to successively emit monochromatic excitation radiation (12, 14) at at least two different excitation wavelengths (λ1, λ2) along a common beam axis (O); an elongated flow section (30) with a longitudinal axis (L) configured to guide a particle stream along the longitudinal axis (L); and an excitation beam path configured to direct the monochromatic excitation radiation (12, 14) into the flow section (30) at a first position (A) and a second position (B), wherein the first position (A) and the second position (B) are located in the flow section (30) and the first position (A) is spaced (Δz) apart from the second position (B).and a detection device (50, 52, 52', 60, 60') configured to selectively filter and detect at least a portion of radiation scattered from the first position (A) at a first filter wavelength (f1) and to selectively filter and detect at least a portion of radiation scattered from the second position (B) at a second filter wavelength (f2).