Speaker
Ms
Soo Mee Kim
(Department of Nuclear Medicine, Seoul National University College of Medicine)
Description
Iterative image reconstruction for Compton camera is computationally challenging
since the projection and backprojection are performed on conical surfaces rather
than along straight lines and there is a number of possible combinations of
position and energy measurements. Therefore, computationally efficient
implementation of a projector-backprojector pair without loss of quantitative
accuracy is required.
Methods: Two different approaches to conical surface integral were investigated for
rapid calculations of an approximately factorized system matrix used for 3-D EM
(expectation maximization) reconstruction: the ellipse-stacking method (ESM) and
the ray-tracing method (RTM). For every possible position in two detectors and
scattering angles, the axis and half angle of the conic surface were determined.
Elements for system matrix were then calculated by the product of differential
cross-section of Compton scattering in scatterer and the probability with which the
voxel belongs to a given conic surface. The belonging probability for ESM was
determined by the distance from the voxel center to the ellipse on a plane parallel
to the scatterer. For RTM, the belonging probability was determined by the
intersection length of the voxel with a straight line through the apex of the cone.
It was assumed that Compton camera consisted of a pair of parallel scatterer and
absorber with 16x16 detector elements in 5x5 cm2 active areas spaced by 5 cm. The
scattering angle of the incident photon at the scatterer was quantized into 30
discrete angles between 10 and 100 degrees. Projection data for point source and
three-cylinder phantom were simulated using both ESM and RTM. The iterative EM
reconstruction algorithms were also implemented using both ESM and RTM. Computation
time (for projections) and percent error between the mathematical phantom and
reconstructed image (64x64x64 matrix with pixel size of 1.56 mm) were compared.
Results: Computation time for projection using ESM was approximately 3 times longer
than RTM. Percent errors (normalized root-mean squared errors) measured at the 30th
iteration for three-cylinder phantom were 44% for ESM and 39% for RTM. Point source
images were well reconstructed by both methods: FWHMs measured by the profile
across the point image reconstructed with 30 iterations were 1.0 pixels for both
methods in the plane parallel to the scatterer, and were 1.3 and 1.8 pixels for ESM
and RTM, respectively, in the plane perpendicular to the scatterer.
Conclusions: Two different approaches to implementing projector-backprojector pairs
for 3-D reconstruction from Compton scattered data were developed. While RTM was
more efficient than ESM in computation time, accuracies of the reconstructions by
both methods were equivalent. The use of geometrical symmetry along with an
efficient caching scheme could greatly reduce the computation time for both
methods.
Author
Ms
Soo Mee Kim
(Department of Nuclear Medicine, Seoul National University College of Medicine)
Co-authors
Prof.
Chan-Hyeong Kim
(Department of Nuclear Engineering, Hanyang University)
Prof.
Chun Sik Lee
(Department of Physics, Chung-Ang University)
Prof.
Dong Soo Lee
(Department of Nuclear Medicine, Seoul National University College of Medicine)
Prof.
Jae Sung Lee
(Department of Nuclear Medicine, Seoul National University College of Medicine)
Dr
Ju Hahn Lee
(Department of Physics, Chung-Ang University)
Ms
Mi No Lee
(Department of Electronic Engineering, Paichai University)
Prof.
Soo-Jin Lee
(Department of Electronic Engineering, Paichai University)