Scattered Radiation Optical Scanner for Transparent Sample Inspection

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Solution Overview

Problem

Current techniques for inspecting thin transparent materials like glass struggle with low reflectivity and high transparency, making it difficult to accurately detect defects, especially in fragile, asymmetric, or large samples, and fail to separate signals from the top and bottom surfaces effectively.

Innovation Solution

An optical scanning system that irradiates the sample at or near the Brewster's angle, using a combination of time-varying beam reflectors and phase retardance detectors to differentiate signals from the top and bottom surfaces, allowing for sensitive defect detection and scanning of various sample shapes and sizes.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Adaptability or versatility

If glass samples are spun for inspection, then defect detection is enabled, but fragile, asymmetric, or large samples cannot be tested

Engineering Contradiction:
Improvesample type compatibilityVSAvoidspinning mechanism requirements
Core Design Contradiction:
Adaptability or versatilityVSDevice complexity

Solution Approach 1:

The patent replaces the mechanical spinning system with a stationary sample holder and uses optical scanning instead. The laser beam is scanned across the sample surface using galvanometer mirrors, eliminating the need for mechanical rotation while still enabling comprehensive defect detection across the entire sample area.

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

Solution Approach 2:

The optical scanning system provides universal applicability to various sample types (fragile, asymmetric, large) by using non-contact optical measurement. The system can inspect any flat surface regardless of its mechanical properties, making it universally applicable to different glass sample configurations without requiring sample rotation.

Inventive Principle:
Principle #6Universality (Multi-functionality)

2Measurement precision

If conventional reflection techniques are used, then defect detection is attempted, but low reflectivity and high transparency of glass make accurate detection difficult

Engineering Contradiction:
Improvedefect detection accuracyVSAvoidsignal detection difficulty
Core Design Contradiction:
Measurement precisionVSDifficulty of detecting and measuring

Solution Approach 1:

The patent changes the optical parameters by using laser light with specific wavelength and polarization, and by controlling the incident angle precisely. These parameter changes enhance the interaction between light and the glass sample, improving the signal strength and detection accuracy despite the low reflectivity of glass.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent introduces phase modulation as an intermediary mechanism. By modulating the phase of the reflected light signal and using lock-in detection, the system enhances the detectability of weak signals from the glass surface, effectively acting as a signal amplifier for low-reflectivity materials.

Inventive Principle:
Principle #24Intermediary (Mediator)

3Measurement precision

If signals from top and bottom surfaces are not separated, then inspection is simpler, but accurate defect localization is impossible

Engineering Contradiction:
Improvedefect localization accuracyVSAvoidsignal separation mechanism
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent segments the reflected light signals into separate components corresponding to reflections from the top surface and bottom surface. By analyzing the temporal and phase characteristics of these segmented signals, the system can distinguish and localize defects on specific surfaces, enabling accurate defect localization.

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 method enhances sensitivity to thin films on transparent samples, enabling accurate detection of defects and film thickness measurements while accommodating diverse sample geometries, improving the inspection process for high-tech products.

Implementation Method 1

a time varying beam reflector that is configured to reflect the light beam through a scan lens towards a transparent sample at an incident angle that is not more than one degree greater or less than Brewster's angle of the transparent sample

Methodology Applied
Scientific EffectReflection: Reflection

Implementation Method 2

measuring phase change in light reflected from the thin transparent material

Methodology Applied
Scientific EffectPhase retardance: Phase Change

Implementation Method 3

A spatial filter is configured to block the second portion of the light beam scattered from the second surface of the transparent sample

Methodology Applied
Scientific EffectScattering: Scattering

Data Source

PatentUS10648928B1Scattered radiation optical scanner
Publication Date: 2020.05.12 LUMINA INSTRUMENTS INC
  • US10648928B1 patent drawing
  • US10648928B1 patent drawing
  • US10648928B1 patent drawing

AI summary

An optical scanning system includes a radiating source capable of outputting a light beam, a time varying beam reflector that is configured to reflect the light beam through a scan lens towards a transparent sample at an incident angle that is not more than one degree greater or less than Brewster's angle of the transparent sample, and a focusing lens configured to be irradiated by light scattered from the transparent sample at an angle that is normal to the plane of incidence of the moving irradiated spot on the transparent sample. A first portion of the light beam is scattered from a first surface of the transparent sample and a second portion of the light beam is scattered from a second surface of the transparent sample. A spatial filter is configured to block the second portion of the light beam scattered from the second surface of the transparent sample.