Physics and Imaging in Radiation Oncology

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Physics and Imaging in Radiation Oncology VOXSI: A voxelized single- and dual-energy CT scenario generator for quantitative imaging  Brent van der Heyden, Lotte E.J.R. Schyns, Mark Podesta, Ana Vaniqui, Isabel P. Almeida, Guillaume Landry, Frank Verhaegen  Physics and Imaging in Radiation Oncology  Volume 6, Pages 47-52 (April 2018) DOI: 10.1016/j.phro.2018.05.004 Copyright © 2018 Maastro Clinic Terms and Conditions

Fig. 1 The flowchart of VOXSI. The X-ray source, simulation geometry, CT setup, and the detector energy response (top row) must be defined before a simulation can be started. After the simulation, the projections are exportable, or can be reconstructed using the implemented ASTRA toolbox and MATLAB’s FBP algorithm. As an alternative, the open-source image reconstruction toolkit (RTK) can be used externally (not implemented in the GUI) to reconstruct the projections (dotted line). The SECT and DECT image analysis toolkit provides tools to analyze the reconstructed CT images. Snapshots of VOXSI’s interface are added in Supplementary material 1. Physics and Imaging in Radiation Oncology 2018 6, 47-52DOI: (10.1016/j.phro.2018.05.004) Copyright © 2018 Maastro Clinic Terms and Conditions

Fig. 2 Comparison of the measured and simulated CT numbers averaged in a circular region of interest (±1 standard deviation (SD)), in Hounsfield Units, for polychromatic 80, 120, and 140 kVp CT X-ray spectra of the RMI 467 soft tissue mimicking inserts (left panel) and the osseous tissue mimicking inserts (middle panel). The right panel plots the absolute differences between the measured and simulated CT numbers for all RMI 467 phantom inserts. Physics and Imaging in Radiation Oncology 2018 6, 47-52DOI: (10.1016/j.phro.2018.05.004) Copyright © 2018 Maastro Clinic Terms and Conditions

Fig. 3 The relative electron density (RED) and effective atomic number (Zeff) calibration curves fitted on the simulated image data of the RMI 467 phantom (left panels) (±1 SD). In the Zeff calibration curve, only 8 of the 11 data points are clearly visible because 3 points closely overlap with another data point. The RED and Zeff images of the simulated XCAT phantom are depicted in the middle panels. The relative differences between the calculated images and the ground truth are shown in the right panels. Physics and Imaging in Radiation Oncology 2018 6, 47-52DOI: (10.1016/j.phro.2018.05.004) Copyright © 2018 Maastro Clinic Terms and Conditions