Atsuro Suzuki1, Wataru Takeuchi2, Takafumi Ishitsu3, Yuichi Morimoto4, Keiji Kobashi5, Yuichiro Ueno6. 1. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. atsuro.suzuki.rc@hitachi.com. 2. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. wataru.takeuchi.rg@hitachi.com. 3. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. takafumi.ishitsu.bb@hitachi.com. 4. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. yuichi.morimoto.fb@hitachi.com. 5. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. keiji.kobashi.xd@hitachi.com. 6. Central Research Laboratory, Hitachi Ltd., 2-1 Omika-cho 7-chome, Hitachi, Ibaraki, 319-1221, Japan. yuichiro.ueno.bv@hitachi.com.
Abstract
OBJECTIVE: To improve the spatial resolution of brain single-photon emission computed tomography (SPECT), we propose a new brain SPECT system in which the detector heads are tilted towards the rotation axis so that they are closer to the brain. In addition, parallel detector heads are used to obtain the complete projection data set. We evaluated this parallel and tilted detector head system (PT-SPECT) in simulations. METHODS: In the simulation study, the tilt angle of the detector heads relative to the axis was 45°. The distance from the collimator surface of the parallel detector heads to the axis was 130 mm. The distance from the collimator surface of the tilted detector heads to the origin on the axis was 110 mm. A CdTe semiconductor panel with a 1.4 mm detector pitch and a parallel-hole collimator were employed in both types of detector head. A line source phantom, cold-rod brain-shaped phantom, and cerebral blood flow phantom were evaluated. The projection data were generated by forward-projection of the phantom images using physics models, and Poisson noise at clinical levels was applied to the projection data. The ordered-subsets expectation maximization algorithm with physics models was used. We also evaluated conventional SPECT using four parallel detector heads for the sake of comparison. RESULTS: The evaluation of the line source phantom showed that the transaxial FWHM in the central slice for conventional SPECT ranged from 6.1 to 8.5 mm, while that for PT-SPECT ranged from 5.3 to 6.9 mm. The cold-rod brain-shaped phantom image showed that conventional SPECT could visualize up to 8-mm-diameter rods. By contrast, PT-SPECT could visualize up to 6-mm-diameter rods in upper slices of a cerebrum. The cerebral blood flow phantom image showed that the PT-SPECT system provided higher resolution at the thalamus and caudate nucleus as well as at the longitudinal fissure of the cerebrum compared with conventional SPECT. CONCLUSION: PT-SPECT provides improved image resolution at not only upper but also at central slices of the cerebrum.
OBJECTIVE: To improve the spatial resolution of brain single-photon emission computed tomography (SPECT), we propose a new brain SPECT system in which the detector heads are tilted towards the rotation axis so that they are closer to the brain. In addition, parallel detector heads are used to obtain the complete projection data set. We evaluated this parallel and tilted detector head system (PT-SPECT) in simulations. METHODS: In the simulation study, the tilt angle of the detector heads relative to the axis was 45°. The distance from the collimator surface of the parallel detector heads to the axis was 130 mm. The distance from the collimator surface of the tilted detector heads to the origin on the axis was 110 mm. A CdTe semiconductor panel with a 1.4 mm detector pitch and a parallel-hole collimator were employed in both types of detector head. A line source phantom, cold-rod brain-shaped phantom, and cerebral blood flow phantom were evaluated. The projection data were generated by forward-projection of the phantom images using physics models, and Poisson noise at clinical levels was applied to the projection data. The ordered-subsets expectation maximization algorithm with physics models was used. We also evaluated conventional SPECT using four parallel detector heads for the sake of comparison. RESULTS: The evaluation of the line source phantom showed that the transaxial FWHM in the central slice for conventional SPECT ranged from 6.1 to 8.5 mm, while that for PT-SPECT ranged from 5.3 to 6.9 mm. The cold-rod brain-shaped phantom image showed that conventional SPECT could visualize up to 8-mm-diameter rods. By contrast, PT-SPECT could visualize up to 6-mm-diameter rods in upper slices of a cerebrum. The cerebral blood flow phantom image showed that the PT-SPECT system provided higher resolution at the thalamus and caudate nucleus as well as at the longitudinal fissure of the cerebrum compared with conventional SPECT. CONCLUSION: PT-SPECT provides improved image resolution at not only upper but also at central slices of the cerebrum.