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@ARTICLE{Pettersen:165909,
author = {H. E. S. Pettersen and L. Volz$^*$ and J. R. Sølie and J.
Alme and G. G. Barnaföldi and R. Barthel and A. van den
Brink and V. Borshchov and M. Chaar and V. N. Eikeland and
G. Genov and O. S. Grøttvik and H. Helstrup and R. Keidel
and C. Kobdaj and N. van der Kolk and S. Mehendale and I.
Meric and O. H. Odland and G. Papp and T. Peitzmann and P.
Piersimoni and M. Protsenko and A. U. Rehman and M. Richter
and A. T. Samnøy and J. Seco$^*$ and H. Shafiee and A.
Songmoolnak and G. Tambave and I. Tymchuk and K. Ullaland
and M. Varga-Kofarago and B. Wagner and R. Xiao and S. Yang
and H. Yokoyama and D. Roehrich},
title = {{H}elium radiography with a digital tracking calorimeter-a
{M}onte {C}arlo study for secondary track rejection.},
journal = {Physics in medicine and biology},
volume = {66},
number = {3},
issn = {1361-6560},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {DKFZ-2020-02466},
pages = {035004},
year = {2021},
note = {2021 Jan 26;66(3):035004},
abstract = {Radiation therapy using protons and heavier ions is a
fast-growing therapeutic option for cancer patients. A
clinical system for particle imaging in particle therapy
would enable online patient position verification,
estimation of the dose deposition through range monitoring
and a reduction of uncertainties in the calculation of the
relative stopping power of the patient. Several prototype
imaging modalities offer radiography and computed tomography
using protons and heavy ions. A Digital Tracking Calorimeter
(DTC), currently under development, has been proposed as one
such detector. In the DTC 43 longitudinal layers of
laterally stacked ALPIDE CMOS monolithic active pixel sensor
chips are able to reconstruct a large number of
simultaneously recorded proton tracks. In this study, we
explored the capability of the DTC for helium imaging which
offers favorable spatial resolution over proton imaging.
Helium ions exhibit a larger cross section for inelastic
nuclear interactions, increasing the number of produced
secondaries in the imaged object and in the detector itself.
To that end, a filtering process able to remove a large
fraction of the secondaries was identified, and the track
reconstruction process was adapted for helium ions. By
filtering on the energy loss along the tracks, on the
incoming angle and on the particle ranges, $97.5\%$ of the
secondaries were removed. After passing through 16 cm water,
$50.0\%$ of the primary helium ions survived; after the
proposed filtering $42.4\%$ of the primaries remained;
finally after subsequent image reconstruction $31\%$ of the
primaries remained. Helium track reconstruction leads to
more track matching errors compared to protons, due to the
increased available focus strength of the helium beam. In a
head phantom radiograph, the Water Equivalent Path Length
error envelope was 1.0 mm for helium and 1.1 mm for protons.
This accuracy is expected to be sufficient for helium
imaging for pre-treatment verification purposes.},
cin = {E041},
ddc = {530},
cid = {I:(DE-He78)E041-20160331},
pnm = {315 - Bildgebung und Radioonkologie (POF4-315)},
pid = {G:(DE-HGF)POF4-315},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:33181502},
doi = {10.1088/1361-6560/abca03},
url = {https://inrepo02.dkfz.de/record/165909},
}