Abstract

We investigated the design of a prompt gamma camera for real-time dose delivery verification and the partial mitigation of range uncertainties. A slit slat (SS) camera was optimized using the trade-off between the signal-to-noise ratio and spatial resolution. Then, using the GATE Monte Carlo package, the camera performances were estimated by means of target shifts, beam position quantification, changing the camera distance from the beam, and air cavity inserting. A homogeneous PMMA phantom and the air gaps induced PMMA phantom were used. The air gaps ranged from 5mm to 30mm by 5mm increments were positioned in the middle of the beam range. To reduce the simulation time, phase space scoring was used. The batch method with five realizations was used for stochastic error calculations. The system's detection efficiency was PGs/proton) for a 10 × 20 cm2 detector (source-to-collimator distance=15.0cm). Axial and transaxial resolutions were 23mm and 18mm, respectively. The SS camera estimated the range as 69.0±3.4 (relative stochastic error 1-sigma is 5%) and 67.6±1.8mm (2.6%) for the real range of 67.0mm for 107 and 108 protons of 100 MeV, respectively. Considering 160 MeV, these values are 155.5±3.1 (2%) and 152.2±2.0mm (1.3%) for the real range of 152.0mm for 107 and 108 protons, respectively. Considering phantom shift, for a 100 MeV beam, the precision of the quantification (1-sigma) in the axial and lateral phantom shift estimation is 2.6mm and 1mm, respectively. Accordingly, the axial and lateral quantification precisions were 1.3mm and 1mm for a 160 MeV beam, respectively. Furthermore, the quantification of an air gap formulated as , where and gapreal are the estimated and real air gap, respectively. The precision of the air gap quantification is 1.6mm (1 sigma). Moreover, 2D PG images show the trajectory of the proton beam through the phantom. The proposed slit-slat imaging systems can potentially provide a real-time, in-vivo, and non-invasive treatment monitoring method for proton therapy.

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