Method and apparatus for compensating for scattering of emission gamma photons for PET imaging

Patent metadata

Field	Value
Publication number	US-9507033-B2
Application number	US-201514688435-A
Country	US
Kind code	B2
Filing date	Apr 16, 2015
Priority date	Feb 5, 2013
Publication date	Nov 29, 2016
Grant date	Nov 29, 2016

Abstract

A process for operating a PET scanner includes acquiring, at a plurality of detector blocks of the PET scanner, emission data of gamma photons of a first energy level originating from annihilation events associated with radioactivity of a phantom in a field of view of the PET scanner. Based on the emission data, an emission block-pair scattering model is generated. The process includes acquiring counts of gamma photons of a second energy level originating from intrinsic background radiation of scintillator crystals of the detector blocks, without any phantom in the field of view, to provide blank scan data for the second energy level. A sinogram is generated based on the blank scan data for the second energy level. The emission block-pair scattering model is added to a scaled version of the sinogram to yield a composite model.

First claim

What is claimed is:

1. A method for operating a positron emission tomography (PET) scanner, the method comprising:
acquiring, at a plurality of detector blocks of the PET scanner, emission data of gamma photons of a first energy level originating from annihilation events associated with radioactivity of a phantom in a field of view of the PET scanner;
based on the emission data, generating an emission block-pair scattering model;
acquiring counts of gamma photons of a second energy level originating from intrinsic background radiation of scintillator crystals of the detector blocks, without any phantom in the field of view, to provide blank scan data for the second energy level;
generating a sinogram based on the blank scan data for the second energy level; and
adding the emission block-pair scattering model to a scaled version of the sinogram, to yield a composite model.

2. The method of claim 1 , wherein generating the emission block-pair scattering model includes:
computing a histogram of counts of gamma photons of the first energy level detected at respective detector blocks over a range of incident angles;
computing a probability of scatter for gamma photons of the first energy level as a function of scattering angle for each pair of detector blocks of the scanner, to obtain a set of scatter probabilities;
computing a probability, for a given scattered gamma photon, of scattering to each detector block in a subset of the plurality of detector blocks, to obtain detector block impact probabilities; and
scaling the computed histogram of counts by the scatter probabilities and the block impact probabilities, to generate the emission block-pair scattering model.

3. The method of claim 1 , further comprising compensating for gamma photons of the first energy level scattering and being detected in an energy window corresponding to the second energy level, said compensating including scaling the composite model.

4. The method of claim 3 , wherein the composite model is scaled based on transmission data of gamma photons of the second energy level, transmission data of gamma photons of a third energy level, the blank scan data for the second energy level, and blank scan data for the third energy level.

5. The method of claim 1 , wherein each detector block impact probability is computed by calculating a solid angle of one detector block from a point of view of another detector block.

6. The method of claim 1 , further comprising:
acquiring transmission data of 307 keV gamma photons originating from intrinsic background radiation of a plurality of scintillator crystals in detector blocks of the PET scanner, when a radioactive phantom is in a field of view of the PET scanner, to provide 307 keV transmission data;
generating a first sinogram based on the 307 keV transmission data;
acquiring counts of 307 keV gamma photons originating from intrinsic background radiation of the scintillator crystals without any phantom in the field of view, to provide 307 keV blank scan data;
generating a second sinogram based on the 307 keV blank scan data; and
automatically comparing the first and second sinograms to generate a scaling mask.

7. The method of claim 6 , further comprising:
acquiring transmission data of 202 keV gamma photons originating from intrinsic background radiation of the scintillator crystals, when the radioactive phantom is in the field of view, to provide 202 keV transmission data;
generating a third sinogram based on the 202 keV transmission data; and
scaling the third sinogram by the scaling mask to generate a set of scale factors.

8. The method of claim 7 , further comprising:
acquiring counts of 202 keV gamma photons originating from intrinsic background radiation of the scintillator crystals without any phantom in the field of view, to provide 202 keV blank scan data;
generating a fourth sinogram based on the 202 keV blank scan data; and
normalizing the fourth sinogram by a mean value of the fourth sinogram, to provide a 202 keV crystal efficiency map.

9. The method of claim 8 , further comprising:
scaling a sum of the emission block-pair scattering model and a scaled version of the fourth sinogram by the 202 keV crystal efficiency map and the scale factors.

10. A method for operating a positron emission tomography (PET) seamier, the method comprising:
acquiring, at a plurality of detector blocks of the PET scanner, emission data of 511 keV gamma photons originating from annihilation events associated with radioactivity of a phantom in a field of view of the PET scanner;
based on the emission data, computing a histogram of counts of 511 keV gamma photons detected at respective detector blocks over a range of incident angles;
computing a probability of scatter for 511 keV gamma photons as a function of scattering angle for each pair of detector blocks of the scanner, to obtain a set of scatter probabilities;
for each detector block, computing a probability, for a given gamma photon scattering at said detector block, of scattering to each other detector block in a subset of the plurality of detector blocks, to provide detector block impact probabilities; and
scaling the computed histogram of counts by the scatter probabilities and the block impact probabilities, to generate an emission block-pair scattering model.

11. A non-transitory machine-readable storage medium, tangibly embodying a program of instructions executable by a system controller to cause the system controller to perform operations comprising:
acquiring, at a plurality of detector blocks of a PET scanner, emission data of gamma photons of a first energy level originating from annihilation events associated with radioactivity of a phantom in a field of view of the PET scanner;
based on the emission data, generating an emission block-pair scattering model;
acquiring counts of gamma photons of a second energy level originating from intrinsic background radiation of scintillator crystals of the detector blocks, without any phantom in the field of view, to provide blank scan data for the second energy level;
generating a sinogram based on the blank scan data for the second energy level; and
adding the emission block-pair scattering model to a scaled version of the sinogram, to yield a composite model.

12. The storage medium of claim 11 , wherein generating the emission block-pair scattering model includes:
computing a histogram of counts of gamma photons of the first energy level detected at respective detector blocks over a range of incident angles;
computing a probability of scatter for gamma photons of the first energy level as a function of scattering angle for each pair of detector blocks of the scanner, to obtain a set of scatter probabilities;
computing a probability, for a given scattered gamma photon, of scattering to each detector block in a subset of the plurality of detector blocks, to obtain detector block impact probabilities; and
scaling the computed histogram of counts by the scatter probabilities and the block impact probabilities, to generate the emission block-pair scattering model.

13. The storage medium of claim 11 , wherein the instructions are further executable by the system controller to cause the system controller to perform operations comprising:
compensating for gamma photons of the first energy level scattering and being detected in an energy window corresponding to the second energy level, said compensating including scaling the composite model.

14. The storage medium of claim 13 , wherein the instructions are executable to cause the system controller to scale the composite model based on transmi

Assignees

• Siemens Medical Solutions Usa Inc
• Siemens Medical Solutions Usa Inc

Inventors

• Rothfuss Harold E
• Panin Vladimir Y

Classifications

• G01T1/1617

  with scintillation detectors (G01T1/20 takes precedence) · CPC title

• G01T1/2985 Primary

  In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis); (using external radiation sources A61B6/02) · CPC title