Radiation Detection with Dual-Threshold Time-Width Analysis

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Solution Overview

Problem

Existing radiation detectors in PET apparatuses face challenges in accurately determining the position of γ-ray interaction due to parallax errors, leading to reduced spatial resolution, especially when the γ-ray is detected away from the detector's center, and current methods for obtaining time waveforms of detection signals are unsuitable for high count rates and high power consumption.

Innovation Solution

A radiation detection device with first and second comparators set to different threshold voltages measures the time widths of digital signals from a scintillator and photodetector, allowing for the determination of a time constant that indicates the time waveform of the detection signal, thereby enabling accurate acquisition and determination of the time waveform with a simple configuration.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If waveform sampling is performed to obtain time waveform information, then measurement precision is improved, but power consumption increases and it becomes unsuitable for high count rate measurement

Engineering Contradiction:
Improvetime waveform measurement precisionVSAvoidpower consumption
Core Design Contradiction:
Measurement precisionVSUse of energy by moving object

Solution Approach 1:

The patent extracts only the essential feature (time width above threshold) from the complete waveform, discarding unnecessary waveform details. This is achieved by comparing the detection signal against a threshold voltage and measuring only the duration above threshold, rather than sampling and storing the entire waveform, thereby reducing power consumption while maintaining measurement precision for time constant determination

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent applies partial action by measuring only the portion of the signal that exceeds the threshold voltage (Time over Threshold), rather than processing the entire waveform. This partial measurement approach provides sufficient information to determine time constants and distinguish scintillator units without the excessive power consumption of complete waveform sampling

Inventive Principle:
Principle #16Partial or excessive action

2Use of energy by moving object

If Time over Threshold (ToT) method is used to obtain detection signal information, then power consumption is reduced, but measurement precision of time constant deteriorates

Engineering Contradiction:
Improvepower consumptionVSAvoidtime constant measurement precision
Core Design Contradiction:
Use of energy by moving objectVSMeasurement precision

Solution Approach 1:

The patent uses the Time over Threshold measurement as an intermediary to indirectly determine the time constant. Instead of directly measuring the complete waveform, the ToT serves as a mediator that, when combined with known threshold voltage and signal amplitude relationships, allows calculation of the time constant with sufficient precision for scintillator unit identification

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The patent changes the measurement parameter from complete waveform sampling to Time over Threshold duration. By measuring the time width above threshold rather than the full waveform shape, the system achieves a balance between power consumption and measurement precision, as the ToT parameter contains sufficient information to determine time constants through mathematical relationships

Inventive Principle:
Principle #35Parameter changes

3Measurement precision

If phoswich type detector with stacked scintillators is used, then spatial resolution is improved, but device complexity increases

Engineering Contradiction:
Improvespatial resolutionVSAvoiddetector structure complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent divides the scintillator into multiple stacked units (first scintillator unit and second scintillator unit) with different time constants. This segmentation allows determination of the interaction depth by identifying which scintillator unit detected the gamma ray based on the time waveform characteristics, thereby improving spatial resolution while maintaining a relatively simple detector structure

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent adds the time dimension to spatial detection by utilizing the different time constants of stacked scintillator units. By measuring the temporal characteristics of the detection signal, the system can determine not only the lateral position but also the depth of interaction, effectively adding a temporal dimension to resolve spatial information without significantly increasing structural complexity

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

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 allows for precise determination of the time waveform of detection signals with reduced power consumption and without the need for complex waveform sampling, supporting high count rates and improved spatial resolution in radiation detection.

Implementation Method 1

a scintillator that generates scintillation light in response to incidence of a radiation ray

Methodology Applied
Scientific EffectScintillation: Scintillation

Implementation Method 2

a photodetector that detects the scintillation light and outputs a detection signal

Methodology Applied
Scientific EffectPhotoelectric effect: Photoelectric Effect

Data Source

PatentEP3644098B1Radiation-detecting device
Publication Date: 2025.09.03 HAMAMATSU PHOTONICS KK
  • EP3644098B1 patent drawingFigure 1
  • EP3644098B1 patent drawingFigure 2
  • EP3644098B1 patent drawingFigure 3

AI summary

A radiation detection device 1A includes a scintillator 11, a photodetector 15 for detecting scintillation light from the scintillator 11 and outputting a detection signal, a first comparator 21 for comparing the detection signal with a first threshold voltage V1 and outputting a signal having a first time width T1, a first time width measurement device 23 for measuring the first time width T1, a second comparator 22 for comparing the detection signal with a second threshold voltage V2 and outputting a signal having a second time width T2, a second time width measurement device 24 for measuring the second time width T2, and an analysis unit 30 for obtaining a time constant τ indicating a time waveform of the detection signal based on the first and second time widths T1 and T2. Thus, it is possible to realize a radiation detection device capable of appropriately acquiring and determining information of a time waveform of a detection signal output from a radiation detector including a scintillator and a photodetector.