Abstract
2150
Objectives Flood sources of 57Co are commonly used for quality control of gamma cameras. Other isotopes, namely 56Co and 58Co, are typical contaminants in commercial flood sources. The half-lives of 56Co (77.2 d) and 58Co (70.9 d) are shorter than that of 57Co (271.7 d), and the flood source becomes purer with time. When a flood source is new, high-energy gamma emissions from 56Co and 58Co may cause tube-pattern non-uniform images. It is thus desirable to develop a simple method to estimate the activity of these contaminants and ensure it meets vendor specifications.
Methods Although minimally present in a flood source, both 56Co and 58Co are positron emitters with branching 19% and 15%, respectively. As is known from 90Y imaging, a clinical PET/CT scanner is capable of imaging weak positron emission in a strong photon background. A 57Co flood source was scanned multiple times over a period of months, acquiring data for 90 minutes per study at a single bed position. Total activity was estimated by measuring average counts per slice in a 80x500mm region of interest, correcting for background counts, and accounting for the positron branching of 56Co and 58Co relative to a reference radionuclide (68Ge/68Ga).
Results Time-of-flight (TOF) PET was found to be necessary for reconstructing suitable images, as non-TOF images could not discern the sheet source from background. The measured positron activity followed exponential behavior with half-life 68 ± 10 days, which is consistent with a mixture of 56Co and 58Co. For this particular flood source, the contaminants at the calibration date were estimated to be 0.05% of initial flood source activity, which is within the manufacturer’s specification of < 0.12%.
Conclusions A clinical TOF PET/CT is effective for imaging the weak positron signal from 56Co and 58Co contaminants in a 57Co flood source. This method provides a simple estimate of flood source purity using available equipment in a clinical setting.