TY - GEN
T1 - Positron range correction in PET using an alternating EM algorithm
AU - Agbeko, Norbert N.
AU - Cheng, Ju Chieh
AU - Laforest, Richard
AU - O'sullivan, Joseph A.
PY - 2010
Y1 - 2010
N2 - In Positron Emission Tomography (PET), positrons travel a short distance before annihilating with an electron resulting in blurred reconstructed imaged because of the difference between the positions of the emitted positrons and their annihilation points. For radionuclides which have a long mean positron range, this results in a significant loss in spatial resolution. This blurring occurs in the image space and is independent of the tomographic imaging process. In this paper we propose a reconstruction algorithm that models the PET imaging problem as a two step process positron emission followed by annihilations which are detected by the imaging system. Within the first step of this approach, the standard EM algorithm for PET is viewed as reconstructing an annihilation distribution rather than the actual activity distribution. Second, the annihilation distribution is then viewed as a blurred version of the activity distribution which can be recovered by image deconvolution with a density dependant positron range kernel. Our proposed algorithm is expressed as an alternating maximization algorithm that maximizes the likelihood of the annihilation and activity distributions given the data.
AB - In Positron Emission Tomography (PET), positrons travel a short distance before annihilating with an electron resulting in blurred reconstructed imaged because of the difference between the positions of the emitted positrons and their annihilation points. For radionuclides which have a long mean positron range, this results in a significant loss in spatial resolution. This blurring occurs in the image space and is independent of the tomographic imaging process. In this paper we propose a reconstruction algorithm that models the PET imaging problem as a two step process positron emission followed by annihilations which are detected by the imaging system. Within the first step of this approach, the standard EM algorithm for PET is viewed as reconstructing an annihilation distribution rather than the actual activity distribution. Second, the annihilation distribution is then viewed as a blurred version of the activity distribution which can be recovered by image deconvolution with a density dependant positron range kernel. Our proposed algorithm is expressed as an alternating maximization algorithm that maximizes the likelihood of the annihilation and activity distributions given the data.
UR - https://www.scopus.com/pages/publications/79960331073
U2 - 10.1109/NSSMIC.2010.5874321
DO - 10.1109/NSSMIC.2010.5874321
M3 - Conference contribution
AN - SCOPUS:79960331073
SN - 9781424491063
T3 - IEEE Nuclear Science Symposium Conference Record
SP - 2875
EP - 2878
BT - IEEE Nuclear Science Symposuim and Medical Imaging Conference, NSS/MIC 2010
T2 - 2010 IEEE Nuclear Science Symposium, Medical Imaging Conference, NSS/MIC 2010 and 17th International Workshop on Room-Temperature Semiconductor X-ray and Gamma-ray Detectors, RTSD 2010
Y2 - 30 October 2010 through 6 November 2010
ER -