Three-Photon Bessel Light Sheet Imaging for Deep Penetration

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Solution Overview

Problem

Conventional light sheet fluorescence microscopy methods face challenges in achieving sufficient image contrast and signal-to-background ratio, especially for larger three-dimensional biological samples, due to high photo-toxicity and scattering issues, which limit the depth of penetration and resolution.

Innovation Solution

A three-photon light sheet imaging system utilizing a non-diffractive, propagation-invariant light sheet, such as a Bessel beam, for three-photon excitation, which reduces scattering and enhances penetration and axial resolution, allowing for lower average intensity levels that minimize sample damage while improving image contrast and signal-to-background ratio.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Illumination intensity

If conventional single-photon or two-photon light sheet illumination is used, then the excitation wavelength is shorter, but the scattering increases and penetration depth is limited

Engineering Contradiction:
Improveexcitation wavelengthVSAvoidscattering
Core Design Contradiction:
Illumination intensityVSObject-affected harmful factors

Solution Approach 1:

The patent changes the excitation wavelength parameter to three-photon excitation (e.g., 1300-1600 nm range), which is three times longer than single-photon excitation. This parameter change reduces Rayleigh scattering by a factor of 81 (since scattering ∝ 1/λ⁴), enabling deeper tissue penetration and improved image contrast

Inventive Principle:
Principle #35Parameter changes

2Area of stationary object

If the light sheet thickness is increased to cover a larger field of view, then the field of view is improved, but the axial resolution deteriorates

Engineering Contradiction:
Improvefield of viewVSAvoidaxial resolution
Core Design Contradiction:
Area of stationary objectVSManufacturing precision

Solution Approach 1:

The patent uses a Bessel beam light sheet which maintains a thin, uniform thickness across a large field of view. The non-diffractive nature of the Bessel beam allows it to preserve its transverse profile over an extended propagation distance, providing consistent axial resolution throughout the entire field of view without requiring the light sheet to be thicker

Inventive Principle:
Principle #3Local quality

3Power

If higher average intensity levels are used for excitation, then the signal strength is improved, but photo-toxicity increases and sample viability is compromised

Engineering Contradiction:
Improvesignal strengthVSAvoidphoto-toxicity
Core Design Contradiction:
PowerVSObject-affected harmful factors

Solution Approach 1:

The patent employs three-photon excitation which allows achieving sufficient signal strength at much lower average intensity levels compared to single- or two-photon excitation. The use of infrared wavelengths (1300-1600 nm) combined with three-photon absorption physics enables excitation with average powers that do not cause photo-toxicity, thereby maintaining sample viability while still providing strong fluorescence signals

Inventive Principle:
Principle #35Parameter changes

4Manufacturing precision

If the light sheet is focused to a thin profile for better axial resolution, then the axial resolution is improved, but the penetration depth into the sample is reduced

Engineering Contradiction:
Improveaxial resolutionVSAvoidpenetration depth
Core Design Contradiction:
Manufacturing precisionVSLength of moving object

Solution Approach 1:

The patent uses a Bessel beam which is generated with a specific annular aperture configuration that creates a non-diffractive light sheet. This preliminary structuring of the light sheet ensures that it maintains its thin profile and high axial resolution over an extended propagation distance, allowing deep penetration while preserving resolution without requiring refocusing at different depths

Inventive Principle:
Principle #10Preliminary action

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 system achieves superior axial resolution and enhanced image contrast across a larger field of view with reduced photo-toxicity, enabling deeper tissue imaging with improved signal-to-background ratio compared to single- or two-photon excitation methods.

Implementation Method 1

an illumination arrangement for generating a light sheet for three-photon excitation of a fluorescent sample

Methodology Applied
Scientific EffectThree-photon excitation: Photoluminescence

Implementation Method 2

Rayleigh scattering is dependent upon 1/λ4. Consequently, the use of three-photon excitation reduces Rayleigh scattering by a factor of 81 when compared with the use of single-photon excitation

Methodology Applied
Scientific EffectRayleigh scattering: Rayleigh Scattering

Implementation Method 3

a fluorescence collection arrangement for collecting fluorescence generated in the sample as a result of three-photon excitation by the light sheet

Methodology Applied
Scientific EffectFluorescence emission: Photoluminescence

Data Source

PatentUS11762180B2Three-photon light sheet imaging
Publication Date: 2023.09.19 UNIV COURT OF THE UNIV OF ST ANDREWS
  • US11762180B2 patent drawing
  • US11762180B2 patent drawing
  • US11762180B2 patent drawing

AI summary

A light sheet imaging system, such as a light sheet microscope, comprises an illumination arrangement for generating a light sheet for three-photon excitation of a fluorescent sample, and a fluorescence collection arrangement for collecting fluorescence generated in the sample as a result of three-photon excitation by the light sheet. The light sheet may be a non-diffractive, propagation-invariant light sheet. The light sheet may be formed from and/or comprise a Bessel beam. A method of light sheet imaging comprises using a light sheet for three-photon excitation of a fluorescent sample, and collecting fluorescence generated in the sample as a result of three-photon excitation of the sample by the light sheet. Such a method may be used for light sheet microscopy.