Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system

<strong>Purpose</strong> Cyclotron-based pencil beam scanning (PBS) proton machines represent nowadays the majority and most affordable choice for proton therapy facilities, however their representation in Monte Carlo (MC) codes is more complex than passively scattered proton system or s...

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Main Authors: Fiorini, F, Schreuder, N, Van den Heuvel, F
Format: Journal article
Published: American Association of Physicists in Medicine 2017
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author Fiorini, F
Schreuder, N
Van den Heuvel, F
author_facet Fiorini, F
Schreuder, N
Van den Heuvel, F
author_sort Fiorini, F
collection OXFORD
description <strong>Purpose</strong> Cyclotron-based pencil beam scanning (PBS) proton machines represent nowadays the majority and most affordable choice for proton therapy facilities, however their representation in Monte Carlo (MC) codes is more complex than passively scattered proton system or synchrotron based PBS machines. This is because degraders are used to decrease the energy from the cyclotron maximum energy to the desired energy, resulting in a unique spot size, divergence and energy spread depending on the amount of degradation. This manuscript outlines a generalized methodology to characterize a cyclotron based PBS machine in a general-purpose MC code. The code can then be used to generate clinically relevant plans starting from commercial TPS plans. <strong>Methods</strong> The described beam is produced at the Provision Proton Therapy Center (Knoxville, Tennessee, USA) using a cyclotron-based IBA Proteus Plus equipment. We characterized the Provision beam in the MC FLUKA using the experimental commissioning data. The code was then validated using experimental data in water phantoms for single pencil beams and larger irregular fields. Comparisons with RayStation TPS plans are also presented. <strong>Results</strong> Comparisons of experimental, simulated and planned dose depositions in water plans show that same doses are calculated by both programs inside the target areas, while penumbrae differences are found at the field edges. These differences are lower for the MC, with a g (3%-3mm) index never below 95%. <strong>Conclusions</strong> Extensive explanations on how MC codes can be adapted to simulate cyclotron based scanning proton machines are given with the aim of using the MC as a TPS verification tool to check and improve clinical plans. For all the tested cases, we showed that dose differences with experimental data are lower for the MC than TPS, implying that the created FLUKA beam model is better able to describe the experimental beam.
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spelling oxford-uuid:c78a3a64-c299-4ab9-87f6-005f69c9c0552022-03-27T06:45:47ZTechnical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo systemJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:c78a3a64-c299-4ab9-87f6-005f69c9c055Symplectic Elements at OxfordAmerican Association of Physicists in Medicine2017Fiorini, FSchreuder, NVan den Heuvel, F<strong>Purpose</strong> Cyclotron-based pencil beam scanning (PBS) proton machines represent nowadays the majority and most affordable choice for proton therapy facilities, however their representation in Monte Carlo (MC) codes is more complex than passively scattered proton system or synchrotron based PBS machines. This is because degraders are used to decrease the energy from the cyclotron maximum energy to the desired energy, resulting in a unique spot size, divergence and energy spread depending on the amount of degradation. This manuscript outlines a generalized methodology to characterize a cyclotron based PBS machine in a general-purpose MC code. The code can then be used to generate clinically relevant plans starting from commercial TPS plans. <strong>Methods</strong> The described beam is produced at the Provision Proton Therapy Center (Knoxville, Tennessee, USA) using a cyclotron-based IBA Proteus Plus equipment. We characterized the Provision beam in the MC FLUKA using the experimental commissioning data. The code was then validated using experimental data in water phantoms for single pencil beams and larger irregular fields. Comparisons with RayStation TPS plans are also presented. <strong>Results</strong> Comparisons of experimental, simulated and planned dose depositions in water plans show that same doses are calculated by both programs inside the target areas, while penumbrae differences are found at the field edges. These differences are lower for the MC, with a g (3%-3mm) index never below 95%. <strong>Conclusions</strong> Extensive explanations on how MC codes can be adapted to simulate cyclotron based scanning proton machines are given with the aim of using the MC as a TPS verification tool to check and improve clinical plans. For all the tested cases, we showed that dose differences with experimental data are lower for the MC than TPS, implying that the created FLUKA beam model is better able to describe the experimental beam.
spellingShingle Fiorini, F
Schreuder, N
Van den Heuvel, F
Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title_full Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title_fullStr Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title_full_unstemmed Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title_short Technical note: Defining cyclotron based clinical scanning proton machines in a FLUKA Monte Carlo system
title_sort technical note defining cyclotron based clinical scanning proton machines in a fluka monte carlo system
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