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@ARTICLE{Oancea:625891,
author = {Oancea, Cristina and Sykorova, Katerina and Jakubek, Jan
and Pivec, Jiri and Riemer, Felix and Worm, Steven and
Bourgouin, Alexandra},
title = {{D}osimetric and temporal beam characterization of
individual pulses in {FLASH} radiotherapy using {T}imepix3
pixelated detector placed out-of-field},
journal = {Physica medica},
volume = {129},
issn = {1120-1797},
address = {Amsterdam},
publisher = {Elsevier},
reportid = {PUBDB-2025-01216},
pages = {104872},
year = {2025},
note = {Waiting for fulltext},
abstract = {Background: FLASH radiotherapy necessitates the development
of advanced Quality Assurance methods and detectors for
accurate monitoring of the radiation field. This study
introduces enhanced time-resolution detection systems and
methods used to measure the delivered number of pulses,
investigate temporal structure of individual pulses and
dose-per-pulse (DPP) based on secondary radiation particles
produced in the experimental room. Methods: A 20 MeV
electron beam generated from a linear accelerator (LINAC)
was delivered to a water phantom. Ultra-high dose-per-pulse
electron beams were used with a dose-per-pulse ranging from
~1 Gy to over 7 Gy. The pulse lengths ranged from 1.18 µs
to 2.88 µs at a pulse rate frequency of 5 Hz. A
semiconductor pixel detector Timepix3 was used to track
single secondary particles. Measurements were performed in
the air, while the detector was positioned out-of-field at a
lateral distance of 200 cm parallel with the LINAC exit
window. The dose deposited was measured along with the pulse
length and the nanostructure of the pulse. Results:The time
of arrival (ToA) of single particles was measured with a
resolution of 1.56 ns, while the deposited energy was
measured with a resolution of several keV based on the Time
over Threshold (ToT) value. The pulse count measured by the
Timepix3 detector corresponded with the delivered values,
which were measured using an in-flange integrating current
transformer (ICT). A linear response (R$^2$ = 0.999) was
established between the delivered beam current and the
measured dose at the detector position (orders of nGy). The
difference between the average measured and delivered pulse
length was ~0.003(30) μs. Conclusion: This simple
non-invasive method exhibits no limitations on the delivered
DPP within the range used during this investigation.},
cin = {$Z_DET$},
ddc = {610},
cid = {$I:(DE-H253)Z_DET-20201126$},
pnm = {622 - Detector Technologies and Systems (POF4-622)},
pid = {G:(DE-HGF)POF4-622},
experiment = {EXP:(DE-H253)PITZ-20150101},
typ = {PUB:(DE-HGF)16},
pubmed = {39667142},
UT = {WOS:001385622400001},
doi = {10.1016/j.ejmp.2024.104872},
url = {https://bib-pubdb1.desy.de/record/625891},
}