Gamma camera, spect device, pet device, and method for generating measured gamma-ray images
US-2015379699-A1 · Dec 31, 2015 · US
US9804275B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9804275-B2 |
| Application number | US-201314084363-A |
| Country | US |
| Kind code | B2 |
| Filing date | Nov 19, 2013 |
| Priority date | Nov 19, 2013 |
| Publication date | Oct 31, 2017 |
| Grant date | Oct 31, 2017 |
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A method and apparatus for generating crystal efficiency correction factors by performing a normalization calibration based on delayed data. The method and apparatus obtain delayed data from a scan of a patient using a Positron Emission Tomography (PET) scanner, generate a sinogram from the obtained delayed data, determine, using a processing circuit, mean fan and block line of response sensitivities from the generated sinogram, determine, using the processing circuit, mean detector efficiency based on the determined mean fan and block line of response sensitivities, determine, using the processing circuit, an individual crystal efficiency based on the determined mean fan and block line of response sensitivities and the mean detector efficiency for each module, and calculate the crystal efficiency correction factors based on the determined individual crystal efficiency of each module.
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The invention claimed is: 1. A method for generating crystal efficiency correction factors by performing a normalization calibration based on delayed data independent of a phantom in a Positron Emission Tomography (PET) apparatus, comprising: obtaining delayed data from a scan of a patient using modules of a PET; generating a sinogram from the obtained delayed data; determining, mean fan response sensitivity and block line response sensitivity based on the generated sinogram by using a processing circuit; determining, using the processing circuit, a mean detector efficiency for each module based on the determined mean fan response sensitivity and block line response sensitivity; determining, using the processing circuit, an individual crystal efficiency of each module based on the determined mean fan response sensitivity and block line response sensitivity and the mean detector efficiency; calculating the crystal efficiency correction factors based on the determined individual crystal efficiency; and calibrating the PET scanner by using the calculated crystal efficiency correction factors to reduce quantitative error and artifacts in image reconstruction by the PET apparatus, wherein each module is a detector having a plurality of crystals, and wherein the obtained delayed data corresponds to patient random paired event data. 2. The method according to claim 1 , wherein the obtaining step further comprises increasing count statistics in delayed-window paired events. 3. The method according to claim 2 , wherein the increasing count statistics comprises one or more selected from a group of increasing a data acquisition FOV, increasing a width of a coincidence window size for delayed window pairing, and increasing a module radiant FOV. 4. The method according to claim 1 , wherein the calculating step comprises calculating the crystal efficiency correction factors including intrinsic crystal efficiency (Ne) and block profile effects (Nb). 5. A method for generating crystal efficiency correction factors by performing a normalization calibration based on delayed data independent of a phantom in a Positron Emission Tomography (PET) apparatus, comprising: obtaining delayed data from modules of a PET scanner; generating a sinogram from the obtained delayed data only; determining, mean fan response sensitivity and block line response sensitivity based on the generated sonogram by using a processing circuit; determining, using the processing circuit, a mean detector efficiency for each module based on the determined mean fan response sensitivity and block line response sensitivity; determining, using the processing circuit, an individual crystal efficiency of each module based on the determined mean fan response sensitivity and block line response sensitivity and the mean detector efficiency; calculating the crystal efficiency correction factors based on the determined individual crystal efficiency; and calibrating the PET scanner by using the calculated crystal efficiency correction factors to reduce quantitative error and artifacts in image reconstruction by the PET apparatus, wherein each module is a detector having a plurality of crystals, and wherein the obtained delayed data corresponds to patient random paired event data. 6. The method according to claim 5 , wherein the obtaining step further comprises increasing count statistics in delayed-window paired events. 7. The method according to claim 6 , wherein the increasing count statistics comprises one or more selected from a group of increasing a data acquisition FOV, increasing a width of a coincidence window size for delayed window pairing, and increasing a module radiant FOV. 8. The method according to claim 5 , wherein the calculating step comprises calculating the crystal efficiency correction factors including intrinsic crystal efficiency (Ne) and block profile effects (Nb). 9. A Positron Emission Tomography (PET) apparatus for generating crystal efficiency correction factors by performing a normalization calibration based on delayed data independent of a phantom, the apparatus comprising: processing circuitry configured to: obtain delayed data from a scan of a patient using modules of a PET scanner; generate a sinogram from the obtained delayed data; determine mean fan response sensitivity and block line response sensitivity based on the generated sonogram by using a processing circuit; determine a mean detector efficiency for each module based on the determined mean fan response sensitivity and block line response sensitivity; determine an individual crystal efficiency of each module based on the determined mean fan response sensitivity and block line response sensitivity and the mean detector efficiency; and calculate the crystal efficiency correction factors based on the determined individual crystal efficiency; and calibrate the PET scanner by using the calculated crystal efficiency correction factors to reduce quantitative error and artifacts in image reconstruction by the PET apparatus, wherein each module is a detector having a plurality of crystals, and wherein the obtained delayed data corresponds to patient random paired event data. 10. The apparatus according to claim 9 , wherein the processing circuitry is configured to increase count statistics in delayed-window paired events. 11. The apparatus according to claim 10 , wherein the processing circuitry is configured to increase count statistics by one or more selected from a group of being configured to increase a data acquisition FOV, being configured to increase a width of a coincidence window size for delayed window pairing, and being configured to increase a module radiant FOV. 12. The apparatus according to claim 9 , wherein the processing circuitry is configured to calculate the crystal efficiency correction factors including intrinsic crystal efficiency (Ne) and block profile effects (Nb). 13. A Positron Emission Tomography (PET) apparatus for generating crystal efficiency correction factors by performing a normalization calibration based on delayed data independent of a phantom, comprising: processing circuitry configured to: obtain delayed data from modules of a PET scanner; generate a sinogram from the obtained delayed data only; determine mean fan response sensitivity and block line response sensitivity based on the generated sonogram by using a processing circuit; determine a mean detector efficiency for each module based on the determined mean fan response sensitivity and block line response sensitivity; determine an individual crystal efficiency of each module based on the determined mean fan response sensitivity and block line response sensitivity and the mean detector efficiency; calculate the crystal efficiency correction factors based on the determined individual crystal efficiency; and calibrate the PET scanner by using the calculated crystal efficiency correction factors to reduce quantitative error and artifacts in image reconstruction by the PET apparatus, wherein each module is a detector having a plurality of crystals, and wherein the obtained delayed data corresponds to patient random paired event data. 14. The apparatus according to claim 13 , wherein the processing circuitry is configured to increase count statistics in delayed-window paired events. 15. The apparatus according to claim 14 , wherein the processing circuitry is configured to increase count statistics by one or more selected from a group of being configured to increase a data acquisition FOV, being configured to increase a width of a coincidence window size for delay
Processing of scintigraphic data (not related to a particular imaging system G01T1/2992) · CPC title
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