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@ARTICLE{Marot:278407,
author = {M. Marot$^*$ and F. Jäger$^*$ and K.-S. Greilich$^*$ and
C. P. Karger$^*$ and O. Jaekel$^*$ and L. N. Burigo$^*$},
title = {{M}onte {C}arlo simulation for proton dosimetry in magnetic
fields: {F}ano test and magnetic field correction factors
k{B}for {F}armer-type ionization chambers.},
journal = {Physics in medicine and biology},
volume = {68},
issn = {0031-9155},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {DKFZ-2023-01641},
pages = {175037},
year = {2023},
note = {#EA:E040#LA:E040# / Phys. Med. Biol. 68 (2023) 175037},
abstract = {In this contribution we present a special Fano test for
charged particles in presence of magnetic fields in the MC
code TOPAS, as well as the determination of magnetic field
correction factors kBfor Farmer-type ionization chambers
using proton $beams.\
\
Approach:$ Customized C++
extensions for TOPAS were implemented to model the special
Fano tests in presence of magnetic fields for electrons and
protons. The Geant4-specific transport
parameters,DRoverRandfinalRange, were investigated to
optimize passing rate and computation time. The kBwas
determined for the Farmer-type PTW 30013 ionization chamber,
and 5 custom built ionization chambers with same geometry
but varying inner radius, testing magnetic flux density
ranging from 0 to 1.0 T and two proton beam energies of
157.43 and 221.05 $MeV.\
\
Main$ results: Using the
investigated parameters, TOPAS passed the Fano test within
$0.39±0.15\%$ and $0.82±0.42\%,$ respectively for
electrons and protons. The chamber response (kBMQ) gives a
maximum at different magnetic flux densities depending of
the chamber size, 1.0043 at 1.0 T for the smallest chamber
and 1.0051 at 0.2 T for the largest chamber. The local dose
difference cBremained ≤ $0.1\%$ for both tested energies.
The magnetic field correction factor kB, for the chamber PTW
30013, varied from 0.9946 to 1.0036 for both tested
$energy.\
\
Significance:$ The developed extension
for the special Fano test in TOPAS MC code with the adjusted
transport parameters, can accurately transport electron and
proton particles in magnetic field. This makes TOPAS a
valuable tool for the determination of kB. The ionization
chambers we tested showed that kBremains small $(<0.7\%).$
To the best of our knowledge, this is the first calculations
of kBfor proton beams. This work represents a significant
step forward in the development of MRgPT and protocols for
proton dosimetry in presence of magnetic $field.\
.$},
keywords = {MR-guided proton therapy (Other) / TOPAS (Other) /
dosimetry (Other) / magnetic field (Other) / magnetic field
correction factor (Other)},
cin = {E040},
ddc = {530},
cid = {I:(DE-He78)E040-20160331},
pnm = {315 - Bildgebung und Radioonkologie (POF4-315)},
pid = {G:(DE-HGF)POF4-315},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:37567226},
doi = {10.1088/1361-6560/acefa1},
url = {https://inrepo02.dkfz.de/record/278407},
}