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Journal of Nuclear Medicine

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Meeting ReportPoster Presentations - Physicians/Scientists/Pharmacists

Integrated imaging now: PET, SPECT, and CT imaging in small animals

Stephen Carcieri, Kyle Kuszpit, Koji Iwata, JoAnn Zhang, Joshua Li, Thor Vandehei, Doug Wagenaar, Kevin Parnham, Brian Ross and Brad Patt
Journal of Nuclear Medicine May 2006, 47 (suppl 1) 399P;
Stephen Carcieri
1Gamma Medica-Ideas, Inc., Northridge, California
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Kyle Kuszpit
2Dept. of Radiology, University of Michigan, Ann Arbor, Michigan
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Koji Iwata
1Gamma Medica-Ideas, Inc., Northridge, California
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JoAnn Zhang
1Gamma Medica-Ideas, Inc., Northridge, California
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Joshua Li
1Gamma Medica-Ideas, Inc., Northridge, California
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Thor Vandehei
1Gamma Medica-Ideas, Inc., Northridge, California
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Doug Wagenaar
1Gamma Medica-Ideas, Inc., Northridge, California
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Kevin Parnham
1Gamma Medica-Ideas, Inc., Northridge, California
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Brian Ross
2Dept. of Radiology, University of Michigan, Ann Arbor, Michigan
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Brad Patt
1Gamma Medica-Ideas, Inc., Northridge, California
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Abstract

1517

Objectives: Ideally, one would like to be able to take PET, SPECT, and CT images in an animal without changing the animal’s position, so that co-registration of images from the different modalities will be highly precise. Here we show that this is possible using the tri-modality FLEX system from Gamma Medica-Ideas, which combines SPECT, PET, and CT imaging systems in a single gantry. The principal challenge in conducting these experiments is the possibility of cross-talk between PET and SPECT. In particular, Compton-scattered gamma rays from F-18 have an energy peak at 170 keV, which is close to the imaging energy window for common SPECT isotopes such as Tc-99m, and can result in noise from F-18 being detected by SPECT cameras. Here we demonstrate that this issue has been overcome with the FLEX system.

Methods: We measured the down-scattered count rate from an F-18 point source into SPECT imaging windows set for Tc-99m. This allowed us to estimate the maximum amount of F-18 that could be injected in an animal without significantly interfering with a SPECT acquisition. We then measured the pile-up count rate into the PET system as a function of the amount of Tc-99m in the PET ring. This allowed us to estimate the maximum amount of Tc-99m that could be injected without interfering with a PET acquisition. Finally, we used these same amounts of activity to acquire SPECT and PET images of a mouse injected with F-18 FDG and Tc-99m MDP.

Results: With a 50 uCi point source of F-18, the down-scattered count rate detected by SPECT cameras was 0.4 kcps. With a 2 mCi point source of Tc-99m, the pile-up count rate detected by the PET ring was 3.2 kcps. PET and SPECT images of a mouse injected with 2 mCi of Tc-99m MDP and 50 uCi of F-18 FDG demonstrated that quality images could be acquired with these amounts of activity.

Conclusions: The high sensitivity of the FLEX PET system allows researchers to use a very small dose of F-18, thus minimizing the down-scattered count rate from F-18 into SPECT imaging energy windows. This, combined with the integration of SPECT, PET, and CT into a single gantry, makes it possible to produce precisely co-registered SPECT, PET, and CT images in small animals.


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Cross-talk between PET and SPECT in the FLEX imaging system.

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Journal of Nuclear Medicine
Vol. 47, Issue suppl 1
May 1, 2006
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Integrated imaging now: PET, SPECT, and CT imaging in small animals
Stephen Carcieri, Kyle Kuszpit, Koji Iwata, JoAnn Zhang, Joshua Li, Thor Vandehei, Doug Wagenaar, Kevin Parnham, Brian Ross, Brad Patt
Journal of Nuclear Medicine May 2006, 47 (suppl 1) 399P;

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Integrated imaging now: PET, SPECT, and CT imaging in small animals
Stephen Carcieri, Kyle Kuszpit, Koji Iwata, JoAnn Zhang, Joshua Li, Thor Vandehei, Doug Wagenaar, Kevin Parnham, Brian Ross, Brad Patt
Journal of Nuclear Medicine May 2006, 47 (suppl 1) 399P;
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