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dc.contributor.author
Maradia, Vivek
dc.contributor.author
Meer, David
dc.contributor.author
Weber, Damien Charles
dc.contributor.author
Lomax, Antony John
dc.contributor.author
Schippers, Jacobus Maarten
dc.contributor.author
Psoroulas, Serena
dc.date.accessioned
2022-01-06T12:18:15Z
dc.date.available
2021-10-30T20:17:43Z
dc.date.available
2021-11-01T07:04:16Z
dc.date.available
2022-01-06T12:18:15Z
dc.date.issued
2021-12
dc.identifier.issn
0094-2405
dc.identifier.issn
2473-4209
dc.identifier.issn
1522-8541
dc.identifier.other
10.1002/mp.15278
en_US
dc.identifier.uri
http://hdl.handle.net/20.500.11850/512857
dc.identifier.doi
10.3929/ethz-b-000512857
dc.description.abstract
Purpose In proton therapy, the potential of using high-dose rates in the cancer treatment is being explored. High-dose rates could improve efficiency and throughput in standard clinical practice, allow efficient utilization of motion mitigation techniques for moving targets, and potentially enhance normal tissue sparing due to the so-called FLASH effect. However, high-dose rates are difficult to reach when lower energy beams are applied in cyclotron-based proton therapy facilities, because they result in large beam sizes and divergences downstream of the degrader, incurring large losses from the cyclotron to the patient position (isocenter). In current facilities, the emittance after the degrader is reduced using circular collimators; however, this does not provide an optimal matching to the acceptance of the following beamline, causing a low transmission for these energies. We, therefore, propose to use a collimation system, asymmetric in both beam size and divergence, resulting in symmetric emittance in both beam transverse planes as required for a gantry system. This new emittance selection, together with a new optics design for the following beamline and gantry, allows a better matching to the beamline acceptance and an improvement of the transmission. Methods We implemented a custom method to design the collimator sizes and shape required to select high emittance, to be transported by the following beamline using new beam optics (designed with TRANSPORT) to maximize acceptance matching. For predicting the transmission in the new configuration (new collimators + optics), we used Monte Carlo simulations implemented in BDSIM, implementing a model of PSI Gantry 2 which we benchmarked against measurements taken in the current clinical scenario (circular collimators + clinical optics). Results From the BDSIM simulations, we found that the new collimator system and matching beam optics results in an overall transmission from the cyclotron to the isocenter for a 70 MeV beam of 0.72%. This is an improvement of almost a factor of 6 over the current clinical performance (0.13% transmission). The new optics satisfies clinical beam requirements at the isocenter. Conclusions We developed a new emittance collimation system for PSI's PROSCAN beamline which, by carefully selecting beam size and divergence asymmetrically, increases the beam transmission for low-energy beams in current state-of-the-art cyclotron-based proton therapy gantries. With these improvements, we could predict almost 1% transmission for low-energy beams at PSI's Gantry 2. Such a system could easily be implemented in facilities interested in increasing dose rates for efficient motion mitigation and FLASH experiments alike.
en_US
dc.format
application/pdf
en_US
dc.language.iso
en
en_US
dc.publisher
Wiley
en_US
dc.rights.uri
http://creativecommons.org/licenses/by-nc-nd/4.0/
dc.subject
Beam Optics
en_US
dc.subject
efficient treatment delivery
en_US
dc.subject
Proton therapy
en_US
dc.subject
FLASH
en_US
dc.subject
Cancer
en_US
dc.subject
Lung cancer
en_US
dc.subject
Liver cancer
en_US
dc.title
A new emittance selection system to maximize beam transmission for low‐energy beams in cyclotron‐based proton therapy facilities with gantry
en_US
dc.type
Journal Article
dc.rights.license
Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International
dc.date.published
2021-10-15
ethz.journal.title
Medical Physics
ethz.journal.volume
48
en_US
ethz.journal.issue
12
en_US
ethz.journal.abbreviated
Med Phys
ethz.pages.start
7613
en_US
ethz.pages.end
7622
en_US
ethz.size
10 p.
en_US
ethz.version.deposit
publishedVersion
en_US
ethz.identifier.wos
ethz.identifier.scopus
ethz.publication.place
s.l.
en_US
ethz.publication.status
published
en_US
ethz.leitzahl
ETH Zürich::00002 - ETH Zürich::00012 - Lehre und Forschung::00007 - Departemente::02010 - Dep. Physik / Dep. of Physics
en_US
ethz.relation.isCitedBy
10.3929/ethz-b-000556701
ethz.relation.isCitedBy
10.3929/ethz-b-000578404
ethz.relation.cites
10.3929/ethz-b-000515078
ethz.date.deposited
2021-10-30T20:17:49Z
ethz.source
FORM
ethz.eth
yes
en_US
ethz.availability
Open access
en_US
ethz.rosetta.installDate
2022-01-06T12:18:38Z
ethz.rosetta.lastUpdated
2022-01-06T12:18:38Z
ethz.rosetta.versionExported
true
ethz.COinS
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