Dispersion-Compensated Optical Coherence Tomography Signal Processing

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Optical coherence tomography (OCT) systems face resolution loss due to dispersion, which blurs boundary surfaces and structures, especially at increasing measuring depths, making it difficult to accurately separate closely adjacent surfaces, and existing dispersion compensation methods are either limited to single depths or require multiple expensive measurements.

Innovation Solution

A device that uses a computer arrangement to detect interference signals, apply dispersion compensation through layer-by-layer phase correction, and perform Fourier transformations to achieve high axial resolution by adapting association instructions for each depth, allowing for section-by-section numeric dispersion compensation.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If dispersion compensation is applied for a single predefined depth, then axial resolution is improved at that specific depth, but the method cannot compensate for dispersion at multiple different depths simultaneously

Engineering Contradiction:
Improveaxial resolutionVSAvoiddepth adaptability
Core Design Contradiction:
Measurement precisionVSAdaptability or versatility

Solution Approach 1:

The patent divides the imaging depth range into multiple depth ranges, with each range requiring separate dispersion compensation. The system processes different depth segments independently, applying appropriate dispersion compensation to each segment to maintain high axial resolution across the entire imaging range.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent implements dynamic dispersion compensation by adjusting compensation parameters according to the specific depth range being processed. The system adapts the dispersion compensation strategy based on the depth position, allowing optimal resolution at each depth rather than using a fixed compensation approach.

Inventive Principle:
Principle #15Dynamics

2Adaptability or versatility

If multiple separate measurements with changed optical compensation are performed for different depths, then dispersion compensation for multiple depths is achieved, but the inherent accuracy of boundary surface position is lost due to multiple measurements

Engineering Contradiction:
Improvemulti-depth compensation capabilityVSAvoidboundary surface position accuracy
Core Design Contradiction:
Adaptability or versatilityVSMeasurement precision

Solution Approach 1:

The patent performs dispersion compensation calculations in advance for multiple depth ranges before actual imaging. By pre-calculating and storing the appropriate compensation parameters for each depth range, the system can quickly apply the correct compensation during imaging without requiring multiple separate measurements, thus maintaining boundary surface position accuracy.

Inventive Principle:
Principle #10Preliminary action

3Measurement precision

If equivalent optical path lengths are generated by introducing identical media in object arm and reference arm, then dispersion compensation is achieved for a single depth, but the system becomes more complex and cannot adapt to different depths

Engineering Contradiction:
Improvedispersion compensation effectivenessVSAvoidoptical path complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent replaces complex optical dispersion compensation mechanisms (introducing physical media in optical paths) with digital signal processing methods. The system uses computer arrangements to calculate and apply dispersion compensation to the interferometric signal, eliminating the need for complex optical components while achieving effective dispersion compensation across multiple depth ranges.

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

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

Enables the detection of boundary surfaces and structures at different depths with high resolution by compensating dispersion specifically for each depth range, resulting in a theoretically highest possible axial resolution in OCT images.

Implementation Method 1

The light scattered back from the object is then superposed by a coherent light beam from a reference arm for obtaining an interference signal

Methodology Applied
Scientific EffectOptical interference: Interference

Implementation Method 2

The object reflects or scatters the light of the light beam into different measuring depths

Methodology Applied
Scientific EffectLight scattering: Scattering

Implementation Method 3

The computer arrangement is designed to determine a plurality of intermediate signals in a spatial frequency range from the interference signal, whereby each of the intermediate signals is dispersion-compensated for a different depth of the object

Methodology Applied
Scientific EffectPhase modulation: Phase Modulation

Implementation Method 4

The computer arrangement is furthermore designed to determine a locally resolved image signal for each of the intermediate signals by applying a Fourier transformation on the particular intermediate signal

Methodology Applied
Scientific EffectFourier transformation:

Data Source

PatentUS9243889B2Device for optical coherence tomography
Publication Date: 2016.01.26 ALCON INC
  • US9243889B2 patent drawing
  • US9243889B2 patent drawing
  • US9243889B2 patent drawing

AI summary

In certain embodiments, a device for optical coherence tomography (OCT) includes a signal detection device and a computer arrangement. The signal detection device is designed to detect an interference signal (G(ω)) for an object to be imaged in an optical frequency range (ω). The computer arrangement is designed to determine intermediate signals (G1(k), G2(k)) in a spatial frequency range (k) from the intermediate interference signal (G(ω)), whereby each of the intermediate signals (G1(k), G2(k)) is dispersion-compensated for a different depth (z1, z2) of the object. A locally resolved image signal (FFT1, FFT2) is determined for each of the intermediate signals (G1(k), G2(k)) by applying a Fourier transformation to the particular intermediate signal (G1(k), G2(k)). A tomography signal (G(z)) is determined from the image signals (FFT1, FFT2).