Quantification of radiotracer uptake with a dedicated breast PET imaging system
Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our...
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| Published in | Medical physics (Lancaster) Vol. 35; no. 11; pp. 4989 - 4997 |
|---|---|
| Main Authors | , , , |
| Format | Journal Article |
| Language | English |
| Published |
United States
American Association of Physicists in Medicine
01.11.2008
|
| Subjects | |
| Online Access | Get full text |
| ISSN | 0094-2405 2473-4209 1522-8541 2473-4209 0094-2405 |
| DOI | 10.1118/1.2990781 |
Cover
| Abstract | Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography–tomography system (PEM–PET). The PEM–PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a
4
×
3
array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a
96
×
72
array of
2
×
2
×
15
mm
3
LYSO detector elements
(
pitch
=
2.1
mm
)
. Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is
15
×
15
×
15
cm
3
. Much of the testing procedures were based on NEMA-NU2/2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of
F
18
concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM–PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. |
|---|---|
| AbstractList | Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography–tomography system (PEM–PET). The PEM–PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4×3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96×72 array of 2×2×15 mm3 LYSO detector elements (pitch=2.1 mm). Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is 15×15×15 cm3. Much of the testing procedures were based on NEMA-NU2∕2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of 18F concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM–PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography–tomography system (PEM–PET). The PEM–PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4×3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96×72 array of 2×2×15mm3 LYSO detector elements (pitch=2.1mm). Image reconstruction is performed with a 3D‐OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field‐of‐view is 15×15×15cm3. Much of the testing procedures were based on NEMA‐NU2/2001 protocols. Count rate losses due to pulse pile‐up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of F18 concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM–PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography–tomography system (PEM–PET). The PEM–PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a array of LYSO detector elements . Image reconstruction is performed with a 3D‐OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field‐of‐view is . Much of the testing procedures were based on NEMA‐NU2/2001 protocols. Count rate losses due to pulse pile‐up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM–PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography–tomography system (PEM–PET). The PEM–PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4 × 3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96 × 72 array of 2 × 2 × 15 mm 3 LYSO detector elements ( pitch = 2.1 mm ) . Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is 15 × 15 × 15 cm 3 . Much of the testing procedures were based on NEMA-NU2/2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of F 18 concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM–PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography-tomography system (PEM-PET). The PEM-PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4 x 3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96 x 72 array of 2 x 2 x 15 mm3 LYSO detector elements (pitch = 2.1 mm). Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is 15 x 15 x 15 cm3. Much of the testing procedures were based on NEMA-NU2/2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of 18F concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM-PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography-tomography system (PEM-PET). The PEM-PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4 x 3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96 x 72 array of 2 x 2 x 15 mm3 LYSO detector elements (pitch = 2.1 mm). Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is 15 x 15 x 15 cm3. Much of the testing procedures were based on NEMA-NU2/2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of 18F concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM-PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments.Tomographic breast imaging techniques can be used to quantify radiotracer uptake in breast and tumor tissue. However, physical processes common to PET imaging can confound accurate quantification. In this investigation, we assessed the effects of these phenomena and tested correction schemes for our new positron emission mammography-tomography system (PEM-PET). The PEM-PET scanner utilizes two sets of rotating planar detector heads. Each unit consists of a 4 x 3 array of Hamamatsu H8500 flat panel position sensitive photomultipliers coupled to a 96 x 72 array of 2 x 2 x 15 mm3 LYSO detector elements (pitch = 2.1 mm). Image reconstruction is performed with a 3D-OSEM algorithm parallelized to run on a multiprocessor computer system. The reconstructed field-of-view is 15 x 15 x 15 cm3. Much of the testing procedures were based on NEMA-NU2/2001 protocols. Count rate losses due to pulse pile-up, image contamination due to acceptance of random coincidences and Compton scatter, and image artifacts produced by photon attenuation were measured. It was found that the system was susceptible to count rate losses when moderate levels of radiation were present in the scanner due to the current design of the event trigger electronics. Application of corrections for Compton scattering, photon attenuation and dead time resulted in improved estimations of 18F concentration in simplified phantom studies. Results from these preliminary studies indicate that the PEM-PET scanner will be useful for the quantification of radiotracer uptake in breast tumors, possibly facilitating early assessment of cancer treatments. |
| Author | Raylman, Raymond R. Smith, Mark F. Kinahan, Paul E. Majewski, Stan |
| Author_xml | – sequence: 1 givenname: Raymond R. surname: Raylman fullname: Raylman, Raymond R. organization: Center for Advanced Imaging, Department of Radiology, West Virginia University, Morgantown, West Virginia 26506-9236 – sequence: 2 givenname: Mark F. surname: Smith fullname: Smith, Mark F. organization: Department of Diagnostic Radiology and Nuclear Medicine, University of Maryland School of Medicine, Baltimore, Maryland 21214 – sequence: 3 givenname: Paul E. surname: Kinahan fullname: Kinahan, Paul E. organization: Department of Radiology, University of Washington, Seattle, Washington 98116 – sequence: 4 givenname: Stan surname: Majewski fullname: Majewski, Stan organization: Radiation Detection and Medical Imaging Group, Thomas Jefferson National Accelerator Facility, Newport News, Virginia 23606 |
| BackLink | https://www.ncbi.nlm.nih.gov/pubmed/19070233$$D View this record in MEDLINE/PubMed |
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| Cites_doi | 10.1109/TNS.1980.4330907 10.1109/23.467880 10.1148/121.2.405 10.1016/j.nima.2006.08.052 10.1118/1.599019 10.1148/radiol.2342040654 10.1088/0031‐9155/53/3/009 10.1088/0031‐9155/41/1/012 10.1148/radiology.189.3.8234714 10.1016/S0001-2998(77)80042-1 10.1177/153303460500400108 10.1097/00004728-198302000-00008 10.1118/1.597169 |
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| Copyright | American Association of Physicists in Medicine 2008 American Association of Physicists in Medicine Copyright © 2008 American Association of Physicists in Medicine 2008 American Association of Physicists in Medicine |
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| Keywords | nuclear medicine breast cancer specialized imagers |
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| Notes | Telephone: (304) 293‐1973; Fax: (304) 293‐4287. rraylman@wvu.edu Author to whom correspondence should be addressed. Electronic mail ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 Author to whom correspondence should be addressed. Electronic mail: rraylman@wvu.edu; Telephone: (304) 293-1973; Fax: (304) 293-4287. |
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| SubjectTerms | Breast - diagnostic imaging Breast - metabolism breast cancer Cancer Compton effect Compton scattering Data acquisition Humans Image detection systems image reconstruction Image scanners Image sensors Mammography medical image processing Medical imaging nuclear medicine Phantoms, Imaging Photons Positron emission tomography (PET) Positron-Emission Tomography Radiation Imaging Physics Radioactive Tracers Radioactivity Reconstruction Sensitivity and Specificity specialized imagers |
| Title | Quantification of radiotracer uptake with a dedicated breast PET imaging system |
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