Swept-Source Raman Spectroscopy Compact Photonic Integration

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Solution Overview

Problem

Conventional Raman spectroscopy systems face tradeoffs between sensitivity, size, and cost, limiting their application in detecting low-concentration biochemicals and requiring larger, more expensive bench-top systems for improved sensitivity.

Innovation Solution

The implementation of a swept source Raman spectroscopy system using a tunable laser with an external cavity photonic integrated circuit, a wavemeter for wavelength measurement, and a large-area detector, which eliminates the need for a spectrometer and enhances sensitivity and compactness.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If a spectrometer is used to improve spectral resolution and sensitivity, then the device size and cost increase

Engineering Contradiction:
Improvespectral resolutionVSAvoiddevice size
Core Design Contradiction:
Measurement precisionVSVolume of stationary object

Solution Approach 1:

The patent extracts the spectral separation function from the traditional spectrometer and implements it through free-space propagation in a compact integrated circuit. This separates the spectral resolution function from the bulky spectrometer hardware, achieving high spectral resolution without the large device size.

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent transitions from two-dimensional spectral separation (using gratings and detectors in traditional spectrometers) to three-dimensional free-space propagation within a photonic integrated circuit. This dimensional change enables spectral resolution without requiring large lateral dimensions.

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

2Measurement precision

If a spectrometer is used to improve detection sensitivity, then the device size and cost increase

Engineering Contradiction:
Improvedetection sensitivityVSAvoiddevice size
Core Design Contradiction:
Measurement precisionVSVolume of stationary object

Solution Approach 1:

The patent extracts the detection function from the traditional spectrometer detector array and implements it using a single photodetector in an integrated circuit. This extraction achieves high detection sensitivity without requiring large detector arrays and associated cooling systems.

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent replaces the mechanical/optical spectrometer system with an integrated photonic circuit that uses free-space propagation for spectral separation. This substitution eliminates the need for moving parts, large optical components, and complex mechanical assemblies while maintaining or improving detection sensitivity.

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

3Measurement precision

If the input slit size is increased to improve detection sensitivity, then the optical path-length must be increased, leading to larger device size

Engineering Contradiction:
Improvedetection sensitivityVSAvoidoptical path-length
Core Design Contradiction:
Measurement precisionVSLength of stationary object

Solution Approach 1:

The patent uses three-dimensional free-space propagation within a compact integrated circuit volume to achieve long effective optical path-lengths without increasing the lateral dimensions or overall device size. The light propagates through multiple layers and dimensions within the chip.

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

Solution Approach 2:

The patent nests the optical path within the integrated circuit structure, allowing the light to traverse a long effective path through multiple functional layers and components that are vertically stacked or spatially arranged within the compact chip footprint.

Inventive Principle:
Principle #7Nested doll (Nesting)

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 achieves higher sensitivity and compactness, enabling the detection of low-concentration biochemicals with improved spectral resolution and reduced size and cost, making Raman spectroscopy more versatile for various applications.

Implementation Method 1

a tunable laser with an external cavity photonic integrated circuit

Methodology Applied
Scientific EffectLaser: Laser

Implementation Method 2

Raman spectroscopy is a technique used to gain information about the chemical composition of a material and the state of that material. In this technique, the sample is illuminated with a bright light source and the wavelength distribution of the scattered light is measured

Methodology Applied
Scientific EffectRaman scattering: Scattering

Implementation Method 3

a wavemeter for wavelength measurement

Methodology Applied
Scientific EffectWavelength measurement:

Implementation Method 4

a large-area detector, which eliminates the need for a spectrometer and enhances sensitivity and compactness

Methodology Applied
Scientific EffectPhotodetection: Photoelectric Effect

Data Source

PatentUS11307092B2Swept-source Raman spectroscopy systems and methods
Publication Date: 2022.04.19 MASSACHUSETTS INST OF TECH
  • US11307092B2 patent drawing
  • US11307092B2 patent drawing
  • US11307092B2 patent drawing

AI summary

In swept source Raman (SSR) spectroscopy, a swept laser beam illuminates a sample, which inelastically scatters some of the incident light. This inelastically scattered light is shifted in wavelength by an amount called the Raman shift. The Raman-shifted light can be measured with a fixed spectrally selective filter and a detector. The Raman spectrum can be obtained by sweeping the wavelength of the excitation source and, therefore, the Raman shift. The resolution of the Raman spectrum is determined by the filter bandwidth and the frequency resolution of the swept source. An SSR spectrometer can be smaller, more sensitive, and less expensive than a conventional Raman spectrometer because it uses a tunable laser and a fixed filter instead of free-space propagation for spectral separation. Its sensitivity depends on the size of the collection optics. And it can use a nonlinearly swept laser beam thanks to a wavemeter that measures the beam's absolute wavelength during Raman spectrum acquisition.