Positron emission tomography systems based on ionization-activated organic fluor molecules, planar pixelated photodetectors, or both

Patent metadata

Field	Value
Publication number	US-12360263-B2
Application number	US-202118033709-A
Country	US
Kind code	B2
Filing date	Oct 26, 2021
Priority date	Oct 28, 2020
Publication date	Jul 15, 2025
Grant date	Jul 15, 2025

Abstract

Gamma-ray detectors for the detection of one or more gamma-rays are provided. Also provided are methods of using the detectors for the detection of one or more gamma-rays. The detectors can be used in high-spatial resolution PET systems, including time-of-flight (TOF)-PET systems. Some of the gamma-ray detectors utilize fluors and an optical imaging system to determine the time and location of a first scattering event of a gamma-ray in a low atomic number scintillating medium. Some of the gamma-ray detectors determine the time and location of a first scattering event of a gamma-ray in a low-density scintillating medium by imaging scintillation photons from the scattering event as a time-series of photon “rings” using a planar pixelated photodetector as a scintillation photon counter.

First claim

What is claimed is:

1. A positron emission tomography system comprising a plurality of imaging modules, the imaging modules comprising:
a scintillator compartment containing a low atomic number scintillating medium comprising one or more fluors, the scintillator compartment having a front face and a back face;
a photodetector system comprising:
one or more photodetectors optically coupled to the scintillator compartment and configured to detect scintillation photons generated in the scintillating medium; and
one or more reflecting surfaces configured to reflect scintillation photons generated in the scintillating medium to the one or more photodetectors;

an optical imaging system comprising:
one or more excitation light sources optically coupled to the scintillator compartment and configured to direct excitation light onto the scintillating medium; and
one or more fluorescence detectors optically coupled to the scintillator compartment and configured to detect fluorescence generated by the fluors in the scintillating medium.

2. The positron emission tomography system of claim 1 , wherein the scintillating medium is a liquid.

3. The positron emission tomography system of claim 1 , wherein the scintillating medium is a solid.

4. The positron emission tomography system of claim 1 , wherein the scintillating medium is a gel.

5. A method for imaging a sample using a positron emission tomography system comprising:
a plurality of imaging modules, the imaging modules comprising:
a scintillator compartment containing a low atomic number scintillating medium comprising one or more fluors, the scintillator compartment having a front face and a back face;
a photodetector system comprising:
one or more photodetectors optically coupled to the scintillator compartment and configured to detect scintillation photons generated in the scintillating medium; and
one or more reflecting surfaces configured to reflect scintillation photons generated in the scintillating medium to the one or more photodetectors;

an optical imaging system comprising:
one or more excitation light sources optically coupled to the scintillator compartment and configured to direct excitation light onto the scintillating medium; and

one or more fluorescence detectors optically coupled to the scintillator compartment and configured to detect fluorescence generated by the fluors in the scintillating medium,
the method comprising:
positioning a sample within an imaging volume defined by the plurality of imaging modules, wherein positron-electron annihilation events in the sample generate coincident gamma-ray pairs;
detecting coincident gamma-ray pairs arriving at a pair of imaging modules using the time-of-flight photodetector system by detecting scintillation photons generated when a first gamma-ray of a coincident gamma-ray pair interacts with the scintillating media in a first imaging module and a second gamma-ray of the coincident gamma-ray pair interacts with the scintillating medium in a second imaging module within a coincidence time window;
initiating a sequence of steps for the first and second imaging modules of each pair of imaging modules that detects a coincident gamma-ray pair, the sequence of steps comprising:
triggering a recording of scintillation light by the time-of-flight photodetector system;
interrogating the scintillating medium by directing excitation light from the one or more excitation light sources onto the scintillating medium, wherein the excitation light excites fluors that have been activated by ionization energy deposited in the scintillating medium by Compton electrons;
recording fluorescence emitted by the excited fluors to generate images of energy clusters corresponding to Compton scatters of the first gamma ray in the scintillating medium of the first imaging module and images of energy clusters corresponding to Compton scatters of the second gamma-ray in the scintillating medium of the second imaging module;
identifying a location of a first collision for the first gamma-ray in the scintillating medium of the first imaging module and a location of a first collision for the second gamma-ray in the scintillating medium of the second imaging module; and
forming a line-of-response between the location of the first collision for the first gamma-ray and the location of the first collision for the second gamma-ray; and
generating an image of a spatial distribution of the positron-electron annihilation events within the sample based on the lines-of-response.

6. The method of claim 5 , wherein the sample is a non-human.

7. The method of claim 5 , wherein the sample is a human.

8. The method of claim 5 , wherein the photodetector system is a time-of-flight photodetector system, and the method further comprises calculating a most likely longitudinal position, and an associated longitudinal resolution of the longitudinal position, for the positron-electron annihilation event along the line-of-response, based on arrival times of the first and second gamma-rays measured by the time-of-flight photodetector system and measurement uncertainties for the locations of the first collisions.

9. The method of claim 8 , wherein the line-of-response is characterized by an initial transverse resolution, and the method further comprises improving the initial transverse resolution of the line-of-response and the longitudinal resolution along the line-of-response based on a totality of spatial information from the images generated by the optical imaging system and temporal information generated by the time-of-flight photodetector system for the Compton scatters of the first and second gamma-rays.

10. The method of claim 5 , further comprising detecting Cherenkov radiation generated when a first gamma-ray of a coincident gamma-ray pair interacts with the scintillating medium in a first imaging module and a second gamma-ray of the coincident gamma-ray pair interacts with the scintillating medium in a second imaging module.

11. The method of claim 5 , wherein the images generated by the optical imaging system provide images of tracks of individual Compton electrons in the scintillating medium, and the images of the tracks reveal one or more of the following track attributes for said Compton electrons: a) an initial Compton-electron direction in the scintillating medium; b) a range of the Compton electron; c) locations of multiple Compton scatters along the track; d) a location of a terminal Compton scatter of the track; and e) total ionization energy deposited by the Compton scatters in the scintillating medium.

12. The method of claim 5 , wherein the images generated by the optical imaging system reveal a direction of a gamma-ray after it undergoes a Compton scatter by identifying an origin of a path of said gamma-ray at said Compton scatter and a termination of the path of said gamma-ray at a location of a subsequent Compton scatter.

13. The method of claim 5 , wherein the step of identifying the location of the first collision for the first gamma-ray in the scintillating medium of the first imaging module and the location of the first collision for the second gamma-ray in the scintillating medium of the second imaging module comprises determining a time-ordering of the Compton scatters of the first and second gamma-rays based on Compton kinematics.

14. The method of claim 13 , wherein application of the Compton kinematics comprises:
calculating a relative probability for each of multiple permutations of a time-ordered chain of successive Compton scatters along paths of the first and second gamma-rays based on relative Compton scatter locations and an

Assignees

• Univ Chicago

Inventors

• Frisch Henry J
• Angelico Evan
• La Riviere Patrick J
• Adams Bernhard W
• Spieglan Eric
• Shida Joao F
• Elagin Andrey
• Domurat-Sousa Kepler
• Squires Allison H

Classifications

• G01T1/1647

  Processing of scintigraphic data (not related to a particular imaging system G01T1/2992) · CPC title

• A61B6/5247

  combining images from an ionising-radiation diagnostic technique and a non-ionising radiation diagnostic technique, e.g. X-ray and ultrasound · CPC title

• A61B6/4258

  for detecting non x-ray radiation, e.g. gamma radiation (A61B6/037 takes precedence) · CPC title

• A61B6/4241

  using energy resolving detectors, e.g. photon counting · CPC title

• A61B6/037 Primary

  Emission tomography · CPC title