Pre-treatment patient-specific stopping power by combining list-mode proton radiography and x-ray CT

被引:31
作者
Collins-Fekete, Charles-Antoine [1 ,2 ,3 ,4 ,5 ]
Brousmiche, Sebastien [6 ]
Hansen, David C. [7 ]
Beaulieu, Luc [1 ,2 ,3 ,4 ]
Seco, Joao [5 ,8 ,9 ]
机构
[1] Univ Laval, Dept Phys Genie Phys & Opt, Quebec City, PQ, Canada
[2] Univ Laval, Ctr Rech Canc, Quebec City, PQ, Canada
[3] CHU Quebec, Dept Radiooncol, Quebec City, PQ, Canada
[4] CHU Quebec, CRCHU Quebec, Quebec City, PQ, Canada
[5] Massachusetts Gen Hosp, Dept Radiat Oncol, Francis H Burr Proton Therapy Ctr, Boston, MA 02114 USA
[6] IBA, Louvain La Neuve, Belgium
[7] Aarhus Univ Hosp, Dept Med Phys, Aarhus, Denmark
[8] Deutsch Krebsforschungszentrum Heidelberg, Baden Wurttemberg, DE, Germany
[9] Heidelberg Univ, Dept Phys & Astron Heidelberg, Baden Wurttemberg, DE, Germany
基金
加拿大创新基金会; 加拿大自然科学与工程研究理事会;
关键词
list-mode proton radiography; x-ray CT; proton stopping power; range uncertainty; proton therapy; proton imaging; Geant4 Monte Carlo; ENERGY COMPUTED-TOMOGRAPHY; EXPERIMENTAL-VERIFICATION; RANGE UNCERTAINTIES; HOUNSFIELD UNITS; PATH FORMALISM; LIKELY PATH; RADIOTHERAPY; THERAPY; CALIBRATION; SIMULATION;
D O I
10.1088/1361-6560/aa7c42
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
The relative stopping power (RSP) uncertainty is the largest contributor to the range uncertainty in proton therapy. The purpose of this work was to develop a systematic method that yields accurate and patient-specific RSPs by combining (1) pre-treatment x-ray CT and (2) daily proton radiography of the patient. The method was formulated as a penalized least squares optimization problem (argmin(parallel to Ax - b parallel to(2)(2))). The parameter A represents the cumulative path-length crossed by the proton in each material, separated by thresholding on the HU. The material RSPs (water equivalent thickness/physical thickness) are denoted by x. The parameter b is the list-mode proton radiography produced using Geant4 simulations. The problem was solved using a non-negative linear-solver with x >= 0. A was computed by superposing proton trajectories calculated with a cubic or linear spline approach to the CT. The material's RSP assigned in Geant4 were used for reference while the clinical HU-RSP calibration curve was used for comparison. The Gammex RMI-467 phantom was first investigated. The standard deviation between the estimated material RSP and the calculated RSP is 0.45%. The robustness of the techniques was then assessed as a function of the number of projections and initial proton energy. Optimization with two initial projections yields precise RSP (<= 1.0%) for 330 MeV protons. 250 MeV protons have shown higher uncertainty (<= 2.0%) due to the loss of precision in the path estimate. Anthropomorphic phantoms of the head, pelvis, and lung were subsequently evaluated. Accurate RSP has been obtained for the head (mu = 0.21 +/- 1.63%), the lung (mu = 0.06 +/- 0.99%) and the pelvis (mu = 0.90 +/- 3.87%). The range precision has been optimized using the calibration curves obtained with the algorithm, yielding a mean R-80 difference to the reference of 0.11 +/- 0.09%, 0.28 +/- 0.34% and 0.05 +/- 0.06% in the same order. The solution's accuracy is limited by the assumed HU/RSP bijection, neglecting inherent degeneracy. The proposed formulation of the problem with prior knowledge x-ray CT demonstrates potential to increase the accuracy of present RSP estimates.
引用
收藏
页码:6836 / 6852
页数:17
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