DocumentCode
1097219
Title
Spatial properties of the scatter response function in SPECT
Author
Frey, E.C. ; Tsui, B.M.W.
Author_Institution
Dept. of Radiol. & Curriculum in Biomed. Eng., North Carolina Univ., Chapel Hill, NC, USA
Volume
38
Issue
2
fYear
1991
fDate
4/1/1991 12:00:00 AM
Firstpage
789
Lastpage
794
Abstract
It was previously shown by the authors (ibid., vol.37, no.3, p.1308-15, 1990) that the scatter response function (SRF) in single photon emission computed tomography (SPECT) imaging can be fit using a fitting function consisting of the sum of a Gaussian and two half-Gaussians with different widths. In the present work, the fitting parameters are studied as a function of source position in a cylindrical water-filled phantom for a low-resolution (LR), high-sensitivity collimator. It is found that each fitting parameter can be described in terms of a single geometric parameter. The useful parameters include the source depth and the distance to the edge of the phantom. However, for a low-energy general-purpose collimator, it may be more useful to parameterize the SRF as the product or other function of the SRF for a semiinfinite slab, and an aperture function which depends on the shape of the surface of the phantom. This parameterization of the SRF is useful for scatter compensation in SPECT
Keywords
computerised tomography; radioisotope scanning and imaging; Gaussian; SPECT; aperture function; cylindrical water-filled phantom; fitting function; geometric parameter; low-resolution high-sensitivity collimator; medical diagnostic imaging; nuclear medicine; parameterization; scatter compensation; scatter response function; semiinfinite slab; single photon emission computed tomography; source depth; source position; Apertures; Biomedical imaging; Collimators; Computational modeling; Computer simulation; Energy resolution; Imaging phantoms; Scattering; Shape; Slabs;
fLanguage
English
Journal_Title
Nuclear Science, IEEE Transactions on
Publisher
ieee
ISSN
0018-9499
Type
jour
DOI
10.1109/23.289392
Filename
289392
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