Validation of a Monte Carlo Framework for Out-of-Field Dose Calculations in Proton Therapy.

Monte Carlo simulation TLD anthropomorphic pediatric phantom bubble detector out-of-field dosimetry proton therapy

Journal

Frontiers in oncology
ISSN: 2234-943X
Titre abrégé: Front Oncol
Pays: Switzerland
ID NLM: 101568867

Informations de publication

Date de publication:
2022
Historique:
received: 23 02 2022
accepted: 04 05 2022
entrez: 27 6 2022
pubmed: 28 6 2022
medline: 28 6 2022
Statut: epublish

Résumé

Proton therapy enables to deliver highly conformed dose distributions owing to the characteristic Bragg peak and the finite range of protons. However, during proton therapy, secondary neutrons are created, which can travel long distances and deposit dose in out-of-field volumes. This out-of-field absorbed dose needs to be considered for radiation-induced secondary cancers, which are particularly relevant in the case of pediatric treatments. Unfortunately, no method exists in clinics for the computation of the out-of-field dose distributions in proton therapy. To help overcome this limitation, a computational tool has been developed based on the Monte Carlo code TOPAS. The purpose of this work is to evaluate the accuracy of this tool in comparison to experimental data obtained from an anthropomorphic phantom irradiation. An anthropomorphic phantom of a 5-year-old child (ATOM, CIRS) was irradiated for a brain tumor treatment in an IBA Proteus Plus facility using a pencil beam dedicated nozzle. The treatment consisted of three pencil beam scanning fields employing a lucite range shifter. Proton energies ranged from 100 to 165 MeV. A median dose of 50.4 Gy(RBE) with 1.8 Gy(RBE) per fraction was prescribed to the initial planning target volume (PTV), which was located in the cerebellum. Thermoluminescent detectors (TLDs), namely, Li-7-enriched LiF : Mg, Ti (MTS-7) type, were used to detect gamma radiation, which is produced by nuclear reactions, and secondary as well as recoil protons created out-of-field by secondary neutrons. Li-6-enriched LiF : Mg,Cu,P (MCP-6) was combined with Li-7-enriched MCP-7 to measure thermal neutrons. TLDs were calibrated in Co-60 and reported on absorbed dose in water per target dose (μGy/Gy) as well as thermal neutron dose equivalent per target dose (μSv/Gy). Additionally, bubble detectors for personal neutron dosimetry (BD-PND) were used for measuring neutrons (>50 keV), which were calibrated in a Cf-252 neutron beam to report on neutron dose equivalent dose data. The Monte Carlo code TOPAS (version 3.6) was run using a phase-space file containing 10

Identifiants

pubmed: 35756661
doi: 10.3389/fonc.2022.882489
pmc: PMC9213663
doi:

Types de publication

Journal Article

Langues

eng

Pagination

882489

Informations de copyright

Copyright © 2022 De Saint-Hubert, Verbeek, Bäumer, Esser, Wulff, Nabha, Van Hoey, Dabin, Stuckmann, Vasi, Radonic, Boissonnat, Schneider, Rodriguez, Timmermann, Thierry-Chef and Brualla.

Déclaration de conflit d'intérêts

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

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Auteurs

Marijke De Saint-Hubert (M)

Research in Dosimetric Applications, Belgian Nuclear Research Center (SCK CEN), Mol, Belgium.

Nico Verbeek (N)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.
Faculty of Medicine, University of Duisburg-Essen, Essen, Germany.

Christian Bäumer (C)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.
Radiation Oncology and Imaging, German Cancer Consortium DKTK, Heidelberg, Germany.
Department of Physics, TU Dortmund University, Dortmund, Germany.

Johannes Esser (J)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.
Faculty of Mathematics and Science Institute of Physics and Medical Physics. Heinrich-Heine University, Düsseldorf, Germany.

Jörg Wulff (J)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.

Racell Nabha (R)

Research in Dosimetric Applications, Belgian Nuclear Research Center (SCK CEN), Mol, Belgium.

Olivier Van Hoey (O)

Research in Dosimetric Applications, Belgian Nuclear Research Center (SCK CEN), Mol, Belgium.

Jérémie Dabin (J)

Research in Dosimetric Applications, Belgian Nuclear Research Center (SCK CEN), Mol, Belgium.

Florian Stuckmann (F)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
Faculty of Mathematics and Science Institute of Physics and Medical Physics. Heinrich-Heine University, Düsseldorf, Germany.
Klinikum Fulda GAG, Universitätsmedizin Marburg, Fulda, Zurich, Germany.

Fabiano Vasi (F)

Physik Institut, Universität Zürich, Zürich, Switzerland.

Stephan Radonic (S)

Physik Institut, Universität Zürich, Zürich, Switzerland.

Guillaume Boissonnat (G)

CEA, Université Paris-Saclay, Palaiseau, France.

Uwe Schneider (U)

Physik Institut, Universität Zürich, Zürich, Switzerland.

Miguel Rodriguez (M)

Hospital Paitilla, Panama City, Panama.
Instituto de Investigaciones Cientificas y de Alta Tecnología INDICASAT-AIP, Panama City, Panama.

Beate Timmermann (B)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.
Faculty of Medicine, University of Duisburg-Essen, Essen, Germany.
Radiation Oncology and Imaging, German Cancer Consortium DKTK, Heidelberg, Germany.
Department of Particle Therapy, University Hospital Essen, Essen, Germany.

Isabelle Thierry-Chef (I)

Radiation Programme, Barcelona Institute for Global Health (ISGlobal), Barcelona, Spain.
University Pompeu Fabra, Barcelona, Spain.
CIBER Epidemiología y Salud Pública, Madrid, Spain.

Lorenzo Brualla (L)

West German Proton Therapy Centre Essen WPE, Essen, Germany.
West German Cancer Center (WTZ), Essen, Germany.
Faculty of Medicine, University of Duisburg-Essen, Essen, Germany.

Classifications MeSH