Abstract:We present a new inversion formula for a weighted conical Radon transform modelling Compton camera data. The formula exploits a large proportion of the acquired events and is easy to implement into fast algorithms. We give for it two equivalent formulations relying on known properties of the two-dimensional Radon transform and we test a semi-iterative algorithm for one of them. From a practical point of view, methods robust to measurement noise and to low number of events are required. We show that adding a co… Show more
“…For the CC analytic algorithm more events were necessary. From 25 × 10 6 simulated events, only one half were usable as a valid Compton cone should not intersect the detector in more than one point, the apex (for details, see reference [45]). A number of 12.5 × 10 6 counts were then simulated for the Anger camera with limited angular coverage.…”
Section: The Sourcementioning
confidence: 99%
“…In this work, we applied the filtered backprojection algorithm developed for CC image reconstruction in [45]. It was shown in [31] that an infinitely large planar detector offers a complete geometry, and the source can be perfectly reconstructed even from only events corresponding to cones with axes perpendicular to that plane.…”
Section: A Filtered Backprojectionmentioning
confidence: 99%
“…This binning reduces the precision on the data and the effect on the image can be remarkable. For instance, a systematic error of 2.5°on the axis inclination will alter the point spread function (PSF) as one moves far from the detector ( [45], Fig. 7).…”
Section: A Filtered Backprojectionmentioning
confidence: 99%
“…Lately, methods accepting a much larger part of the data were developed ( [35], [36], [37], [38]). The conical Radon transform is born and is receiving much interest ( [39], [40], [41], [42], [43], [44], [45], [46]).…”
Compton cameras and collimated gamma cameras are competing devices suitable for prompt gamma detection in range verification of particle therapy. In this study, we evaluate the first approach from the point of view of the tomographic reconstruction step by comparing it to the second. We clear any technological constraints by considering a simple geometry, ideal detecting stages, a mono-energetic synthetic phantom. To this end, both analytic (filtered backprojection) and iterative (maximum likelihood expectation maximization) algorithms are applied in conjunction with total variation denoising. The results we obtain show that the collimated configuration leads to slightly better images when the same number of acquired events is used for the reconstruction. However, the Compton camera might equal the collimator-based camera if we take into account the superior efficiency and might surpass it in a limited angle configuration when the collimated camera cannot span the entire angular range.
“…For the CC analytic algorithm more events were necessary. From 25 × 10 6 simulated events, only one half were usable as a valid Compton cone should not intersect the detector in more than one point, the apex (for details, see reference [45]). A number of 12.5 × 10 6 counts were then simulated for the Anger camera with limited angular coverage.…”
Section: The Sourcementioning
confidence: 99%
“…In this work, we applied the filtered backprojection algorithm developed for CC image reconstruction in [45]. It was shown in [31] that an infinitely large planar detector offers a complete geometry, and the source can be perfectly reconstructed even from only events corresponding to cones with axes perpendicular to that plane.…”
Section: A Filtered Backprojectionmentioning
confidence: 99%
“…This binning reduces the precision on the data and the effect on the image can be remarkable. For instance, a systematic error of 2.5°on the axis inclination will alter the point spread function (PSF) as one moves far from the detector ( [45], Fig. 7).…”
Section: A Filtered Backprojectionmentioning
confidence: 99%
“…Lately, methods accepting a much larger part of the data were developed ( [35], [36], [37], [38]). The conical Radon transform is born and is receiving much interest ( [39], [40], [41], [42], [43], [44], [45], [46]).…”
Compton cameras and collimated gamma cameras are competing devices suitable for prompt gamma detection in range verification of particle therapy. In this study, we evaluate the first approach from the point of view of the tomographic reconstruction step by comparing it to the second. We clear any technological constraints by considering a simple geometry, ideal detecting stages, a mono-energetic synthetic phantom. To this end, both analytic (filtered backprojection) and iterative (maximum likelihood expectation maximization) algorithms are applied in conjunction with total variation denoising. The results we obtain show that the collimated configuration leads to slightly better images when the same number of acquired events is used for the reconstruction. However, the Compton camera might equal the collimator-based camera if we take into account the superior efficiency and might surpass it in a limited angle configuration when the collimated camera cannot span the entire angular range.
“…Once the optimal solution is found, we apply a TVregularization [20], which is used in Compton imaging with other algorithms [21], in order to denoise the source space image by minimizing ‖∇ ‖ � .…”
Compton imaging is one of the main methods to localize radioactive hotspots, which emit high-energy gamma-ray photons, above 200 keV. Most of the Compton imaging systems are composed by at least two detection layers or one 3D position sensitive detector. In this study, we demonstrate the application of a new miniature pixelated single plane detector to Compton imaging. In this configuration, we do not have the information on interaction depth but we successfully test its ability to perform Compton localization by means of comparing different Compton reconstruction algorithms applied to real data measured with our single plane detection system.
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