Premium
Variance‐based sensitivity analysis for uncertainties in proton therapy: A framework to assess the effect of simultaneous uncertainties in range, positioning, and RBE model predictions on RBE‐weighted dose distributions
Author(s) -
Hofmaier Jan,
Dedes George,
Carlson David J.,
Parodi Katia,
Belka Claus,
Kamp Florian
Publication year - 2021
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1002/mp.14596
Subject(s) - proton therapy , pencil beam scanning , bragg peak , range (aeronautics) , relative biological effectiveness , monte carlo method , nuclear medicine , proton , particle therapy , radiation treatment planning , histogram , voxel , sensitivity (control systems) , mathematics , computational physics , physics , statistics , beam (structure) , computer science , radiation therapy , materials science , irradiation , nuclear physics , optics , medicine , artificial intelligence , radiology , electronic engineering , engineering , composite material , image (mathematics)
Purpose Treatment plans in proton therapy are more sensitive to uncertainties than in conventional photon therapy. In addition to setup uncertainties, proton therapy is affected by uncertainties in proton range and relative biological effectiveness (RBE). While to date a constant RBE of 1.1 is commonly assumed, the actual RBE is known to increase toward the distal end of the spread‐out Bragg peak. Several models for variable RBE predictions exist. We present a framework to evaluate the combined impact and interactions of setup, range, and RBE uncertainties in a comprehensive, variance‐based sensitivity analysis (SA). Material and methods The variance‐based SA requires a large number (10 4 –10 5 ) of RBE‐weighted dose (RWD) calculations. Based on a particle therapy extension of the research treatment planning system CERR we implemented a fast, graphics processing unit (GPU) accelerated pencil beam modeling of patient and range shifts. For RBE predictions, two biological models were included: The mechanistic repair‐misrepair‐fixation (RMF) model and the phenomenological Wedenberg model. All input parameters (patient position, proton range, RBE model parameters) are sampled simultaneously within their assumed probability distributions. Statistical formalisms rank the input parameters according to their influence on the overall uncertainty of RBE‐weighted dose–volume histogram (RW‐DVH) quantiles and the RWD in every voxel, resulting in relative, normalized sensitivity indices (S = 0: noninfluential input, S = 1: only influential input). Results are visualized as RW‐DVHs with error bars and sensitivity maps. Results and conclusions The approach is demonstrated for two representative brain tumor cases and a prostate case. The full SA including ∼ 3 × 10 4RWD calculations took 39, 11, and 55 min, respectively. Range uncertainty was an important contribution to overall uncertainty at the distal end of the target, while the relatively smaller uncertainty inside the target was governed by biological uncertainties. Consequently, the uncertainty of the RW‐DVH quantile D 98 for the target was governed by range uncertainty while the uncertainty of the mean target dose was dominated by the biological parameters. The SA framework is a powerful and flexible tool to evaluate uncertainty in RWD distributions and DVH quantiles, taking into account physical and RBE uncertainties and their interactions. The additional information might help to prioritize research efforts to reduce physical and RBE uncertainties and could also have implications for future approaches to biologically robust planning and optimization.