ML-EM based dual tracer PET image reconstruction with inclusion of prompt gamma attenuation

被引:0
|
作者
Pfaehler, Elisabeth [1 ]
Niekaemper, Debora [1 ]
Scheins, Juergen [1 ]
Shah, N. Jon [1 ,2 ,3 ,4 ]
Lerche, Christoph W. [1 ]
机构
[1] Forschungszentrum Julich, Inst Neurosci & Med 4, INM 4, Julich, Germany
[2] Forschungszentrum Julich, Inst Neurosci & Med 11, JARA, INM 11, Julich, Germany
[3] JARA BRAIN Translat Med, Aachen, Germany
[4] Rhein Westfal TH Aachen, Dept Neurol, Aachen, Germany
来源
PHYSICS IN MEDICINE AND BIOLOGY | 2025年 / 70卷 / 01期
关键词
positron emission tomography; dual tracer PET; maximum-likelihood expectation maximization; IN-VIVO; ISOTOPE;
D O I
10.1088/1361-6560/ad9660
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
Objective. Conventionally, if two metabolic processes are of interest for image analysis, two separate, sequential positron emission tomography (PET) scans are performed. However, sequential PET scans cannot simultaneously display the metabolic targets. The concurrent study of two simultaneous PET scans could provide new insights into the causes of diseases. Approach. In this work, we propose a reconstruction algorithm for the simultaneous injection of a beta+-emitter emitting only annihilation photons and a beta+-gamma-emitter emitting annihilation photons and an additional prompt gamma-photon. As in previous works, the gamma-photon is used to identify events originating from the beta+-gamma-emitter. However, due to e.g. attenuation and down-scatter, the gamma-photon is often not detected and not all events can correctly be associated with the beta+-gamma-emitter as they are detected as double coincidences. In contrast to previous works, we estimate this number of double coincidences with origin in the beta+-gamma, emitter including the attenuation of the prompt gamma, and incorporate this estimation in the forward-projection of the maximum likelihood expectation maximization algorithm. For evaluation, we simulate different scenarios with varying objects and attenuation maps. The nuclide 18F serves as beta+-emitter, while 44Sc functions as beta+-gamma emitter. The performance of the algorithm is assessed by calculating the residual error of the beta+-gamma-emitter in the reconstructed beta+-emitter image. Additionally, the intensity values in the simulated cylinders of the ground truth (GT) and the reconstructed images are compared. Main results. The remaining activity in the beta+-emitter image varied from 0.4% to 3.7%. The absolute percentage difference between GT and reconstructed intensity for the pure beta+ emitter images was found to be between 3.0% and 7.4% for all cases. The absolute percentage difference between the GT and the reconstructed intensity for the beta+-gamma emitter images ranged from 8.7% to 10.4% for all simulated cases. Significance. These results demonstrate that our approach can reconstruct two separate images with a good quantitation accuracy.
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页数:16
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