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@ARTICLE{Kretschmer:274231,
author = {J. Kretschmer and L. Brodbek and C. Behrends and F. Kugel
and B. Koska and C. Bäumer$^*$ and J. Wulff and B.
Timmermann$^*$ and B. Poppe and H. K. Looe},
title = {{C}omprehensive investigation of lateral dose profile and
output factor measurements in small proton fields from
different delivery techniques.},
journal = {Medical physics},
volume = {50},
number = {7},
issn = {0094-2405},
address = {College Park, Md.},
publisher = {AAPM},
reportid = {DKFZ-2023-00517},
pages = {4546-4561},
year = {2023},
note = {2023 Jul;50(7):4546-4561},
abstract = {As part of the commissioning and quality assurance in
proton beam therapy, lateral dose profiles and output
factors have to be acquired. Such measurements can be
performed with point detectors and are especially
challenging in small fields or steep lateral penumbra
regions as the detector's volume effect may lead to
perturbations. To address this issue, this work aims to
quantify and correct for such perturbations of six point
detectors in small proton fields created via three different
delivery techniques.Lateral dose profile and output
measurements of three proton beam delivery techniques
(pencil beam scanning, pencil beam scanning combined with
collimators, passive scattering with collimators) were
performed using high-resolution EBT3 films, a PinPoint 3D
31022 ionization chamber, a microSilicon diode 60023 and a
microDiamond detector 60019 (all PTW Freiburg, Germany).
Detector specific lateral dose response functions K(x,y)
acting as the convolution kernel transforming the
undisturbed dose distribution D(x,y) into the measured
signal profiles M(x,y) were applied to quantify
perturbations of the six investigated detectors in the
proton fields and correct the measurements. A signal
theoretical analysis in Fourier space of the dose
distributions and detector's K(x,y) was performed to aid the
understanding of the measurement process with regard to the
combination of detector choice and delivery
technique.Quantification of the lateral penumbra broadening
and signal reduction at the fields center revealed that
measurements in the pencil beam scanning fields are only
compromised slightly even by large volume ionization
chambers with maximum differences in the lateral penumbra of
0.25 mm and $4\%$ signal reduction at the field center. In
contrast, radiation techniques with collimation are not
accurately represented by the investigated detectors as
indicated by a penumbra broadening up to 1.6 mm for passive
scattering with collimators and 2.2 mm for pencil beam
scanning with collimators. For a 3 mm diameter collimator
field, a signal reduction at field center between $7.6\%$
and $60.7\%$ was asserted. Lateral dose profile measurements
have been corrected via deconvolution with the corresponding
K(x,y) to obtain the undisturbed D(x,y). Corrected output
ratios of the passively scattered collimated fields obtained
for the microDiamond, microSilicon and PinPoint 3D show
agreement better than $0.9\%$ (one standard deviation) for
the smallest field size of 3 mm.Point detector perturbations
in small proton fields created with three delivery
techniques were quantified and found to be especially
pronounced for collimated small proton fields with steep
dose gradients. Among all investigated detectors, the
microSilicon diode showed the smallest perturbations. The
correction strategies based on detector's K(x,y) were found
suitable for obtaining unperturbed lateral dose profiles and
output factors. Approximation of K(x,y) by considering only
the geometrical averaging effect has been shown to provide
reasonable prediction of the detector's volume effect. The
findings of this work may be used to guide the choice of
point detectors in various proton fields and to contribute
towards the development of a code of practice for small
field proton dosimetry. This article is protected by
copyright. All rights reserved.},
keywords = {lateral penumbra (Other) / output factors (Other) / proton
fields (Other) / small field dosimetry (Other) / volume
effect (Other)},
cin = {ED01},
ddc = {610},
cid = {I:(DE-He78)ED01-20160331},
pnm = {899 - ohne Topic (POF4-899)},
pid = {G:(DE-HGF)POF4-899},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:36908165},
doi = {10.1002/mp.16357},
url = {https://inrepo02.dkfz.de/record/274231},
}