Adam Farag1,2,3, R Terry Thompson4,5,6, Jonathan D Thiessen4,5,7,6, Frank S Prato4,5,7,8,6, Jean Théberge4,5,7,8,6. 1. Lawson Health Research Institute, Imaging Division, London, Ontario, Canada. adam.farag@uwo.ca. 2. Department of Medical Biophysics, Western University, London, Ontario, Canada. adam.farag@uwo.ca. 3. Lawson Imaging Division, St. Joseph's Health Care London, 268 Grosvenor St., PO Box 5777, STN B, London, ON, N6A 4V2, Canada. adam.farag@uwo.ca. 4. Lawson Health Research Institute, Imaging Division, London, Ontario, Canada. 5. Department of Medical Biophysics, Western University, London, Ontario, Canada. 6. Lawson Imaging Division, St. Joseph's Health Care London, 268 Grosvenor St., PO Box 5777, STN B, London, ON, N6A 4V2, Canada. 7. Department of Medical Imaging, Western University, London, Ontario, Canada. 8. St. Joseph`s Health Care, Diagnostic Imaging, London, Ontario, Canada.
Abstract
BACKGROUND: Accurate quantification of radioactivity, measured by an integrated positron emission tomography (PET) and magnetic resonance imaging (MRI) system, is still a challenge. One aspect of such a challenge is to correct for the hardware attenuation, such as the patient table and radio frequency (RF) resonators. For PET/MRI systems, computed tomography (CT) is commonly used to produce hardware attenuation correction (AC) maps, by converting Hounsfield units (HU) to a linear attenuation coefficients (LAC) map at the PET energy level 511 keV, using a bilinear model. The model does not address beam hardening, nor higher density materials, which can lead to inaccurate corrections. PURPOSE: In this study, we introduce a transmission-based (TX-based) AC technique with a static Germanium-68 (Ge-68) transmission source to generate hardware AC maps using the PET/MRI system itself, without the need for PET or medical CT scanners. The AC TX-based maps were generated for a homogeneous cylinder, made of acrylic as a validator. The technique thereafter was applied to the patient table and posterior part of an RF-phased array used in cardiovascular PET/MRI imaging. The proposed TX-based, and the CT-based, hardware maps were used in reconstructing PET images of one cardiac patient, and the results were analysed and compared. RESULTS: The LAC derived by the TX-based method for the acrylic cylinder is estimated to be 0.10851 ± 0.00380 cm-1 compared to the 0.10698 ± 0.00321 cm-1 theoretical value reported in the literature. The PET photon counts were reduced by 8.7 ± 1.1% with the patient table, at the region used in cardiac scans, while the CT-based map, used for correction, over-estimated counts by 4.3 ± 1.3%. Reconstructed in vivo images using TX-based AC hardware maps have shown 4.1 ± 0.9% mean difference compared to those reconstructed images using CT-based AC. CONCLUSIONS: The LAC of the acrylic cylinder measurements using the TX-based technique was in agreement with those in the literature confirming the validity of the technique. The over-estimation of photon counts caused by the CT-based model used for the patient table was improved by the TX-based technique. Therefore, TX-based AC of hardware using the PET/MRI system itself is possible and can produce more accurate images when compared to the CT-based hardware AC in cardiac PET images.
BACKGROUND: Accurate quantification of radioactivity, measured by an integrated positron emission tomography (PET) and magnetic resonance imaging (MRI) system, is still a challenge. One aspect of such a challenge is to correct for the hardware attenuation, such as the patient table and radio frequency (RF) resonators. For PET/MRI systems, computed tomography (CT) is commonly used to produce hardware attenuation correction (AC) maps, by converting Hounsfield units (HU) to a linear attenuation coefficients (LAC) map at the PET energy level 511 keV, using a bilinear model. The model does not address beam hardening, nor higher density materials, which can lead to inaccurate corrections. PURPOSE: In this study, we introduce a transmission-based (TX-based) AC technique with a static Germanium-68 (Ge-68) transmission source to generate hardware AC maps using the PET/MRI system itself, without the need for PET or medical CT scanners. The AC TX-based maps were generated for a homogeneous cylinder, made of acrylic as a validator. The technique thereafter was applied to the patient table and posterior part of an RF-phased array used in cardiovascular PET/MRI imaging. The proposed TX-based, and the CT-based, hardware maps were used in reconstructing PET images of one cardiac patient, and the results were analysed and compared. RESULTS: The LAC derived by the TX-based method for the acrylic cylinder is estimated to be 0.10851 ± 0.00380 cm-1 compared to the 0.10698 ± 0.00321 cm-1 theoretical value reported in the literature. The PET photon counts were reduced by 8.7 ± 1.1% with the patient table, at the region used in cardiac scans, while the CT-based map, used for correction, over-estimated counts by 4.3 ± 1.3%. Reconstructed in vivo images using TX-based AC hardware maps have shown 4.1 ± 0.9% mean difference compared to those reconstructed images using CT-based AC. CONCLUSIONS: The LAC of the acrylic cylinder measurements using the TX-based technique was in agreement with those in the literature confirming the validity of the technique. The over-estimation of photon counts caused by the CT-based model used for the patient table was improved by the TX-based technique. Therefore, TX-based AC of hardware using the PET/MRI system itself is possible and can produce more accurate images when compared to the CT-based hardware AC in cardiac PET images.
Authors: Ciprian Catana; Richard Laforest; Hongyu An; Fernando Boada; Tuoyu Cao; David Faul; Bjoern Jakoby; Floris P Jansen; Bradley J Kemp; Paul E Kinahan; Peder Larson; Michael A Levine; Piotr Maniawski; Osama Mawlawi; Jonathan E McConathy; Alan B McMillan; Julie C Price; Abhejit Rajagopal; John Sunderland; Patrick Veit-Haibach; Kristen A Wangerin; Chunwei Ying; Thomas A Hope Journal: J Nucl Med Date: 2021-07-22 Impact factor: 11.082