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The Journal of Nuclear Medicine Vol. 21 No. 10 971-977
© 1980 by Society of Nuclear Medicine
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Method for Optimizing Side Shielding in Positron-Emission Tomographs and for Comparing Detector Materials

Stephen E. Derenzo

University of California, Berkeley, California

Correspondence: For reprints contact: Stephen E. Derenzo, PhD, Donner Laboratory, University of California, Berkeley, CA 94720.

ABSTRACT

This report presents analytical formulas for the image-forming and background event rates seen by circular positron-emission tomographs with parallel side shielding. These formulas include deadtime losses, detector efficiency, coincidence resolving time, amount of activity, patient port diameter, shielding gap, and shielding depth. A figure of merit, defined in terms of these quantities, describes the signal-to-noise ratio in the reconstructed image of a 20-cm cylinder of water with uniformly dispersed activity. For 1-cm-wide NaI(Tl) detectors, a 50-cm patient port, an activity of 200 µCl per axial centimeter, and a shielding gap of 2 cm, the optimum shielding depth is 20 cm, which requires a detector circle diameter of 90 cm. For a 25-cm patient port and other conditions as above, the optimum shielding depth is 14 cm. Results are presented for the scintillators NaI(Tl), bismuth germanate (BGO), CsF, and plastic; and for Ge(Li) and wire chambers with converters. In these examples, BGO provided the best signal-to-noise for activity levels below 1000 µCi per cm, and CsF had the advantage for higher activity levels.







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Copyright © 1980 by the Society of Nuclear Medicine.