Fluorescence Microscope Time-Gated Detection for Stray Light Crosstalk

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Solution Overview

Problem

Fluorescent microscopes suffer from stray excitation light leakage onto the detector, which overwhelms faint fluorescence signals, reducing the signal-to-noise ratio and obscuring fine details, particularly in sensitive applications like medical diagnostics and cellular biology research.

Innovation Solution

An optical system with a time-gated detector array that selectively directs excitation and detection light using a beam splitter, and gates the detector array to avoid crosstalk by recording detection signals only outside excitation light pulses, utilizing a control unit to integrate and process detection signals efficiently.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If beam splitters and spectral filters are used to combine and separate excitation and detection light, then the optical system can function, but the system becomes technically complex and excitation light leakage still occurs

Engineering Contradiction:
Improveprevention of excitation light leakageVSAvoidoptical system complexity
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The excitation light source operates in pulsed mode rather than continuous mode. The detector is synchronized to detect signals only during specific time windows after each excitation pulse, thereby separating excitation and detection in time. This temporal modulation eliminates the need for complex beam splitters and spectral filters while preventing excitation light leakage.

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The patent transitions from separating light paths spatially (using beam splitters and filters in the optical path) to separating them temporally (using pulsed excitation and time-gated detection). This adds the time dimension to the light path separation problem, simplifying the optical components required.

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

2Measurement precision

If excitation light intensity is increased to improve signal strength, then detection sensitivity improves, but stray light leakage overwhelms the detector and reduces signal-to-noise ratio

Engineering Contradiction:
Improvesignal-to-noise ratioVSAvoidstray excitation light impact
Core Design Contradiction:
Measurement precisionVSObject-affected harmful factors

Solution Approach 1:

By using pulsed excitation light and time-gated detection, the system can use high excitation intensity during the pulse while only detecting during the darker intervals between pulses. This temporal separation allows high power excitation without overwhelming the detector with stray light, improving signal-to-noise ratio.

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The patent converts the harmful effect of high excitation light intensity (which causes stray light leakage) into a beneficial temporal signature. The pulsed nature of the excitation allows the detector to identify and capture only the fluorescence signal that occurs after each pulse, while ignoring the excitation light itself and any scattered excitation photons.

Inventive Principle:
Principle #22Blessing in disguise (Convert harm into benefit)

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 signal-to-noise ratio and improves image quality by reducing excitation light crosstalk, enabling high-resolution detection and efficient data processing, especially in fluorescence microscopy.

Implementation Method 1

The detector array is time-gated with respect to the pulses of the excitation light

Methodology Applied
Scientific EffectTime-gating:

Implementation Method 2

a beam splitter configured to direct the excitation light from the excitation light source to the objective lens and to direct the detection light from the objective lens to the detection unit

Methodology Applied
Scientific EffectLight reflection and transmission: Reflection

Implementation Method 3

an objective lens configured to direct the excitation light into a sample space and to receive detection light from the sample space

Methodology Applied
Scientific EffectLight focusing: Lens

Implementation Method 4

a scanner arranged between the excitation light source and the objective lens and configured to selectively direct the excitation light into different regions of the sample space via the objective lens

Methodology Applied
Scientific EffectLight deflection: Reflection

Implementation Method 5

an excitation light source configured to generate pulses of excitation light

Methodology Applied
Scientific EffectLight emission: Laser

Implementation Method 6

a detection unit comprising a detector array and configured to receive the detection light

Methodology Applied
Scientific EffectFluorescence detection: Fluorescence

Data Source

PatentUS20250370240A1Optical system for a microscope and a method for operating the microscope
Publication Date: 2025.12.04 LEICA MICROSYSTEMS CMS GMBH
  • US20250370240A1 patent drawing
  • US20250370240A1 patent drawing
  • US20250370240A1 patent drawing

AI summary

An optical system for a microscope includes an excitation light source configured to generate pulses of excitation light, an objective lens configured to direct the excitation light into a sample space and to receive detection light from the sample space, a detection unit comprising a detector array and configured to receive the detection light, a scanner arranged between the excitation light source and the objective lens and configured to selectively direct the excitation light into different regions of the sample space via the objective lens, and a beam splitter configured to direct the excitation light from the excitation light source to the objective lens and to direct the detection light from the objective lens to the detection unit. The detector array is time-gated with respect to the pulses of the excitation light.