Optimizing cone beam CT scatter estimation in egs_cbct for a clinical and virtual chest phantom

被引:17
作者
Thing, Rune Slot [1 ,2 ]
Mainegra-Hing, Ernesto [3 ]
机构
[1] Univ Southern Denmark, Inst Clin Res, DK-5000 Odense, Denmark
[2] Odense Univ Hosp, Lab Radiat Phys, DK-5000 Odense, Denmark
[3] Natl Res Council Canada, Ottawa, ON K1A 0R6, Canada
关键词
Monte Carlo; EGSnrc; CBCT imaging; image quality; x-ray scatter; variance reduction techniques; MONTE-CARLO-SIMULATION;
D O I
10.1118/1.4881142
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
Purpose: Cone beam computed tomography (CBCT) image quality suffers from contamination from scattered photons in the projection images. Monte Carlo simulations are a powerful tool to investigate the properties of scattered photons. egs_cbct, a recent EGSnrc user code, provides the ability of performing fast scatter calculations in CBCT projection images. This paper investigates how optimization of user inputs can provide the most efficient scatter calculations. Methods: Two simulation geometries with two different x-ray sources were simulated, while the user input parameters for the efficiency improving techniques (EITs) implemented in egs_cbct were varied. Simulation efficiencies were compared to analog simulations performed without using any EITs. Resulting scatter distributions were confirmed unbiased against the analog simulations. Results: The optimal EIT parameter selection depends on the simulation geometry and x-ray source. Forced detection improved the scatter calculation efficiency by 80%. Delta transport improved calculation efficiency by a further 34%, while particle splitting combined with Russian roulette improved the efficiency by a factor of 45 or more. Combining these variance reduction techniques with a built-in denoising algorithm, efficiency improvements of 4 orders of magnitude were achieved. Conclusions: Using the built-in EITs in egs_cbct can improve scatter calculation efficiencies by more than 4 orders of magnitude. To achieve this, the user must optimize the input parameters to the specific simulation geometry. Realizing the full potential of the denoising algorithm requires keeping the statistical uncertainty below a threshold value above which the efficiency drops exponentially. (C) 2014 American Association of Physicists in Medicine.
引用
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页数:7
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