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On scatter in megavoltage x‐ray transmission imaging (in English)
Author(s) -
Spies Lothar
Publication year - 2000
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 - 10.1118/1.598905
Subject(s) - monte carlo method , imaging phantom , optics , physics , photon , detector , beam (structure) , range (aeronautics) , computational physics , materials science , mathematics , statistics , composite material
This thesis considers the role of scatter in electronic portal imaging devices (EPIDs). The thesis involved a direct measurement of scatter in an EPID. An already established Monte Carlo code, developed at the Royal Marsden Hospital, Sutton/UK, was extended and agreed with the experimental data for phantom‐to‐detector distances larger than 10 cm. An analytical scatter model was developed on the basis of the Monte Carlo analysis. In this model scatter was estimated by convolving the input beam profile with an analytical scatter kernel. The model was tested over a wide range of clinical parameters. For a 6 MV x‐ray beam impinging upon a water‐equivalent phantom, the absolute error in the scatter‐to‐primary ratio was better than 1% for a 100 cm 2field. The accuracy dropped to 4% for a 400 cm 2field. The model was implemented for a camera‐based EPID with a converter comprising a 1‐mm‐thick copper plate bonded to a 134 mg / cm 2phosphor foil. Algorithms were developed for correcting for scatter contributions in megavoltage CT (MVCT) and for reconstruction of input beam profiles. For the latter an overall accuracy of better than 4% was obtained for fields of 100 cm 2in size. In MVCT the yield in contrast resolution after a scatter correction was small. However, a scatter correction reduced the discrepancy of 30% between true and reconstructed electron densities to 10%. In both applications the limit in accuracy is a direct consequence of the performance of the converter, which strongly overestimates multiply scattered photons of low energy. Within the framework of a convolution model multiply scattered radiation exiting an inhomogeneous phantom cannot be calculated with an accuracy exceeding the limits given.