Liquid Xenon Argon Positron Detector for Hadrotherapy

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Solution Overview

Problem

Current positron emission tomography (PET) and Time Of Flight (TOF-PET) units have limited radial resolution, high tracer doses, poor image contrast and brightness, and inefficient γ-ray detection due to sub-optimal scintillators and detectors, leading to increased radiation exposure, especially in pediatric patients, and inability to accurately monitor dose delivery to cancer cells versus healthy tissues.

Innovation Solution

A detector unit with a hollow body containing a scintillating material like liquid argon or xenon with fast decay time, high atomic number, and high scintillation yield, paired with photo-detecting units and shielding to enhance radial resolution and Signal-to-Noise Ratio, allowing for reduced tracer doses and improved image clarity, and integration with hadrotherapy machines for precise dose monitoring.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If inorganic scintillators (LSO, LYSO) are used in commercial TOF-PET units, then detection sensitivity is improved, but radial resolution deteriorates to a few cm due to slow scintillation decay times (40-80 ns)

Engineering Contradiction:
Improvedetection sensitivityVSAvoidradial resolution
Core Design Contradiction:
ReliabilityVSMeasurement precision

Solution Approach 1:

The patent changes the key parameter of scintillation decay time from 40-80 ns (inorganic scintillators) to less than 10 ns (liquid scintillators), enabling both high detection sensitivity and excellent radial resolution (4-5 mm) to be achieved simultaneously

Inventive Principle:
Principle #35Parameter changes

2Loss of information

If tomographic reconstruction is used to produce three-dimensional images, then image completeness is improved, but radiation dose increases due to the need for high tracer activity (10 mCi, 12 mSv per procedure)

Engineering Contradiction:
Improveimage completenessVSAvoidradiation dose
Core Design Contradiction:
Loss of informationVSObject-affected harmful factors

Solution Approach 1:

The patent replaces the indirect tomographic reconstruction method with direct three-dimensional imaging capability, allowing complete spatial information to be obtained without requiring high tracer activities, thereby reducing radiation dose to patients

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

3Reliability

If inorganic scintillators with thick crystals are used, then gamma-ray detection efficiency is improved, but manufacturing cost and device complexity increase

Engineering Contradiction:
Improvegamma-ray detection efficiencyVSAvoiddetector structure complexity
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The patent uses liquid scintillators (fluid state) instead of solid inorganic scintillator crystals, simplifying the detector structure while maintaining high gamma-ray detection efficiency through the fluid's ability to fully contain interaction volumes

Inventive Principle:
Principle #29Pneumatics and hydraulics

Data Source

PatentUS10314551B2Detector, three-dimensional direct positron imaging unit, and method to estimate the differential of the radiation dose provided to cancer cells and healthy tissues during hadrotherapy
Publication Date: 2019.06.11 THE TRUSTEES OF PRINCETON UNIV
  • US10314551B2 patent drawing
  • US10314551B2 patent drawing
  • US10314551B2 patent drawing

AI summary

Disclosed is a detector for a positron imaging unit, comprises a hollow body with an inner cylindrical wall and an outer wall spaced apart from the inner cylindrical wall. The hollow body includes a scintillating material, suitable to emit photons once hit by a 511 keV γ-ray, and one or more pairs of photo-detecting units (e.g. comprising PMTs or SiPM) for detecting photons emitted by the scintillating material; each photo-detecting unit of a pair being placed at opposite ends of the inner cylindrical wall along a radial direction. The scintillating material has scintillation decay time τ lower than 10 ns, an atomic number greater than 10, and a high scintillation yield greater than 8,000 photons/MeV, and comprises a mixture of xenon and argon. An imaging unit including the detector and a method to estimate the differential of the dose of radiation provided in a subject to cancer cells and to surrounding tissues in the course of hadrotherapy is also disclosed.