Scintillator Crystal Light Sharing for PET DOI Estimation

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Solution Overview

Problem

Current PET detector systems face challenges in accurately estimating the depth of interaction (DOI) of gamma photons, leading to parallax error and reduced timing and spatial resolution, particularly due to the use of larger crystal arrays with broader light sharing which affects timing resolution and increases computational complexity.

Innovation Solution

A photon detector scintillator arrangement with a 2x2 array of scintillator crystal bars, where each crystal is optically coupled to a sensor, and light sharing is implemented between adjacent crystals, allowing for efficient DOI estimation using look-up tables (LUTs) constructed during calibration, which simplifies the computation and maintains high timing resolution.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If larger crystal arrays with broader light sharing are used to improve DOI estimation, then measurement precision of DOI is improved, but timing resolution deteriorates and device complexity increases

Engineering Contradiction:
ImproveDOI estimation accuracyVSAvoidtiming resolution
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The patent divides the crystal array into smaller 2x2 blocks, where light sharing is performed only within each block rather than across the entire array. This segmentation maintains DOI estimation capability while limiting light sharing scope to preserve timing resolution and reduce computational burden.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent implements light sharing with different characteristics in different regions: within the 2x2 block, light sharing enables DOI estimation, while between blocks, optical isolation preserves timing resolution. This local differentiation resolves the contradiction by applying light sharing only where needed for DOI measurement.

Inventive Principle:
Principle #3Local quality

2Measurement precision

If larger crystal arrays with continuous DOI measurement are used, then measurement precision of DOI is improved, but device complexity and computational complexity increase

Engineering Contradiction:
ImproveDOI estimation accuracyVSAvoidcomputation complexity
Core Design Contradiction:
Measurement precisionVSDevice complexity

Solution Approach 1:

The patent segments the DOI measurement problem into discrete 2x2 block units, each with its own lookup table. This segmentation reduces computational complexity by avoiding global optimization across the entire crystal array, while still providing accurate DOI estimation at each local block level.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent performs DOI calibration and generates lookup tables in advance during system setup, rather than computing DOI in real-time during photon detection. This preliminary action significantly reduces computational complexity during actual operation while maintaining measurement precision.

Inventive Principle:
Principle #10Preliminary action

3Device complexity

If fixed center point between crystal surfaces is used for LOR endpoints, then device complexity is reduced, but measurement precision deteriorates due to parallax error

Engineering Contradiction:
Improvesystem simplicityVSAvoidLOR localization accuracy
Core Design Contradiction:
Device complexityVSMeasurement precision

Solution Approach 1:

The patent replaces the mechanical/geometric approach of using fixed crystal surface centers with an optical field-based approach using light sharing ratios. The DOI is determined by analyzing how scintillation light distributes between adjacent crystals, providing accurate localization without requiring complex mechanical adjustments or fixed reference points.

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

This arrangement provides excellent timing and spatial resolution while simplifying the computation of DOI, reducing parallax error and maintaining high system throughput, even in ring detector configurations.

Implementation Method 1

The gamma photon interacts with the molecules within the crystal, which converts the gamma photon or scintillates to generate luminescence

Methodology Applied
Scientific EffectScintillation: Scintillation

Implementation Method 2

The generated luminescence or light is sensed by an optical sensor located on an opposite crystal face from the center facing surface. The crystals are typically long, rectangular bars with the smaller end center facing surface receiving the gamma photon, and with the opposite smaller end surface coupled to one or more optical sensors, which convert the sensed luminescence to an energy value and a time value measuring the received gamma photon

Methodology Applied
Scientific EffectPhotoelectric Effect: Photoelectric Effect

Data Source

PatentEP3207406B1Pet detector scintillator arrangement with light sharing and depth of interaction estimation
Publication Date: 2020.07.29 KONINKLIJKE PHILIPS NV
  • EP3207406B1 patent drawingFigure 1
  • EP3207406B1 patent drawingFigure 2A~2B
  • EP3207406B1 patent drawingFigure 3A~3B

AI summary

A photon detector includes a sensor array of optical sensors disposed in a plane and four substantially identical scintillation crystal bars. Each optical sensor is configured to sense luminescence. Each of the four scintillator crystal bars being a rectangular prism with four side surfaces and first and second end surfaces, each scintillation bar has two side surfaces which each face a side surface of another scintillation bar, and each scintillation crystal bar generating a light scintillation in response to interacting with a received gamma photon. A first layer (80) is disposed in a first plane disposed between and adjacent facing side surfaces of the four substantially identical scintillation crystal bars with a light sharing portion (82) adjacent the first end surface and a reflective portion (84) adjacent the second end surface. A second layer (68) is disposed in a second plane orthogonal to the first plane and disposed between and adjacent facing side surfaces of the four substantially identical scintillation crystal bars with a light sharing portion (88) adjacent the second end surface and a reflective portion (90) adjacent the first end surface.