Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator

An integrated system of a linear accelerator and a magnetic resonance imaging (MRI) device may provide real-time imaging during radiotherapy treatments. This work investigated changes affecting the dose deposition caused by a magnetic field (B-field) transverse to the beam direction by means of Mont...

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Main Authors: Richter Sebastian, Pojtinger Stefan, Mönnich David, Dohm Oliver S., Thorwarth Daniela
Format: Article
Language:English
Published: De Gruyter 2017-09-01
Series:Current Directions in Biomedical Engineering
Subjects:
Online Access:https://doi.org/10.1515/cdbme-2017-0058
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author Richter Sebastian
Pojtinger Stefan
Mönnich David
Dohm Oliver S.
Thorwarth Daniela
author_facet Richter Sebastian
Pojtinger Stefan
Mönnich David
Dohm Oliver S.
Thorwarth Daniela
author_sort Richter Sebastian
collection DOAJ
description An integrated system of a linear accelerator and a magnetic resonance imaging (MRI) device may provide real-time imaging during radiotherapy treatments. This work investigated changes affecting the dose deposition caused by a magnetic field (B-field) transverse to the beam direction by means of Monte Carlo simulations. Two different phantoms were used: A water phantom (Ph1) and a water-air phantom (Ph2) with a 4-2-4 cm water-air-water cross section. Dose depositions were scored for B-field values of 0 T, 0.35 T, 0.5 T, 1.5 T, 3 T and 5 T. Beams were based on a precalculated photon spectrum taken from an earlier simulated Elekta 6 MV FFF accelerator. All lateral profiles in Ph1 showed a Lorentz force driven shift w.r.t. the B-field strength, presenting a steeper penumbra in the shift's direction. Depositions were shifted up to 0.3 cm for 5 T, showing a constant central axis plateau-dose or an increase by 2.3 % for small fields. Depth-dose curves in Ph1 showed a shift of the dose maximum towards the beam entrance direction for increasing B-field of up to 1.1 cm; the maximum dose was increased by 6.9 %. In Ph2, an asymmetric dose increase by up to 36.9 % was observed for 1.5 T at the water-air boundary, resulting from the electron return effect (ERE). In our scenario, B-field dependent dose shifts and local build-ups were observed, which consequently affect the resulting dose distribution and need to be considered in magnetic resonance guided radiotherapy treatment planning.
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spelling doaj.art-20a9ccf2595045e2a69abaaa86536cc42023-04-11T17:07:13ZengDe GruyterCurrent Directions in Biomedical Engineering2364-55042017-09-013228128510.1515/cdbme-2017-0058cdbme-2017-0058Influence of a transverse magnetic field on the dose deposited by a 6 MV linear acceleratorRichter Sebastian0Pojtinger Stefan1Mönnich David2Dohm Oliver S.3Thorwarth Daniela4University Hospital Tübingen, Department of Radiation Oncology, Section for Biomedical Physics, Hoppe-Seyler-Str. 3, 72076 Tübingen, GermanyUniversity Hospital Tübingen, Department of Radiation Oncology, Section for Biomedical Physics, Hoppe-Seyler-Str. 3, 72076 Tübingen, GermanyUniversity Hospital Tübingen, Department of Radiation Oncology, Section for Biomedical Physics, Hoppe-Seyler-Str. 3, 72076 Tübingen, GermanyUniversity Hospital Tübingen, Department of Radiation Oncology, Division for Medical Physics, Hoppe-Seyler-Str. 3, 72076 Tübingen, GermanyUniversity Hospital Tübingen, Department of Radiation Oncology, Section for Biomedical Physics, Hoppe-Seyler-Str. 3, 72076 Tübingen, GermanyAn integrated system of a linear accelerator and a magnetic resonance imaging (MRI) device may provide real-time imaging during radiotherapy treatments. This work investigated changes affecting the dose deposition caused by a magnetic field (B-field) transverse to the beam direction by means of Monte Carlo simulations. Two different phantoms were used: A water phantom (Ph1) and a water-air phantom (Ph2) with a 4-2-4 cm water-air-water cross section. Dose depositions were scored for B-field values of 0 T, 0.35 T, 0.5 T, 1.5 T, 3 T and 5 T. Beams were based on a precalculated photon spectrum taken from an earlier simulated Elekta 6 MV FFF accelerator. All lateral profiles in Ph1 showed a Lorentz force driven shift w.r.t. the B-field strength, presenting a steeper penumbra in the shift's direction. Depositions were shifted up to 0.3 cm for 5 T, showing a constant central axis plateau-dose or an increase by 2.3 % for small fields. Depth-dose curves in Ph1 showed a shift of the dose maximum towards the beam entrance direction for increasing B-field of up to 1.1 cm; the maximum dose was increased by 6.9 %. In Ph2, an asymmetric dose increase by up to 36.9 % was observed for 1.5 T at the water-air boundary, resulting from the electron return effect (ERE). In our scenario, B-field dependent dose shifts and local build-ups were observed, which consequently affect the resulting dose distribution and need to be considered in magnetic resonance guided radiotherapy treatment planning.https://doi.org/10.1515/cdbme-2017-0058radiotherapymagnetic fieldmonte carlo simulationdose depositionerelinear acceleratormrgrtmr-linac
spellingShingle Richter Sebastian
Pojtinger Stefan
Mönnich David
Dohm Oliver S.
Thorwarth Daniela
Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
Current Directions in Biomedical Engineering
radiotherapy
magnetic field
monte carlo simulation
dose deposition
ere
linear accelerator
mrgrt
mr-linac
title Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
title_full Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
title_fullStr Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
title_full_unstemmed Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
title_short Influence of a transverse magnetic field on the dose deposited by a 6 MV linear accelerator
title_sort influence of a transverse magnetic field on the dose deposited by a 6 mv linear accelerator
topic radiotherapy
magnetic field
monte carlo simulation
dose deposition
ere
linear accelerator
mrgrt
mr-linac
url https://doi.org/10.1515/cdbme-2017-0058
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