001     289482
005     20250826101727.0
024 7 _ |a 10.1016/j.radmeas.2024.107097
|2 doi
024 7 _ |a 1350-4487
|2 ISSN
024 7 _ |a 1879-0925
|2 ISSN
037 _ _ |a DKFZ-2024-00804
041 _ _ |a English
082 _ _ |a 530
100 1 _ |a Schmidt, Stefan
|0 P:(DE-He78)f726c09d369bb3767687f686aa6694fb
|b 0
|e First author
|u dkfz
245 _ _ |a Converter thickness optimisation using Monte Carlo simulations of Fluorescent Nuclear Track Detectors for neutron dosimetry
260 _ _ |a Amsterdam [u.a.]
|c 2024
|b Elsevier Science
336 7 _ |a article
|2 DRIVER
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|b journal
|m journal
|0 PUB:(DE-HGF)16
|s 1713351094_10702
|2 PUB:(DE-HGF)
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a Journal Article
|0 0
|2 EndNote
500 _ _ |a #EA:E040#LA:E040#
520 _ _ |a Secondary neutrons generated during ion beam radiotherapy present a concern due to the potential dosedeposition beyond the treatment volume, thereby elevating the risk of inducing secondary tumours. Theseneutrons can possess energies comparable to those of the primary ions, reaching magnitudes of severalhundred MeV, posing a challenge for neutron detectors. Fluorescent Nuclear Track Detectors (FNTDs) arepromising detectors for high-energy neutron dosimetry given their capability to detect particles with a lowlinear energy transfer. In this work, the sensitivity of FNTDs to neutron energies reaching 20 MeV was analysedby experiments and Monte Carlo (MC) simulations, quantifying the recoil proton yield of FNTDs combinedwith polyethylene (PE) converters of different thicknesses. The FNTDs were read out using a dedicated FNTDreader, demonstrating a reasonable uncertainty by analysing a detector area of 0.1 mm2. Investigations ofdifferent converter thicknesses reveal optimal detector sensitivity between 0.5 mm to 1.0 mm for a 241AmBesource, yielding a maximum sensitivity of (22.7±3.4) tracks mSv−1 mm−2. Similar converter-FNTD configurationswere assessed through MC simulations using FLUKA, yielding a correlation between detector sensitivity andconverter thickness. Furthermore, an enhanced detector sensitivity for neutron energies up to 20 MeV wasfound for the PE converter thickness of 4.0 mm. The MC simulations can be used to optimise FNTD detectorconfigurations for measuring higher neutron energies by maximising the recoil proton yield.
536 _ _ |a 315 - Bildgebung und Radioonkologie (POF4-315)
|0 G:(DE-HGF)POF4-315
|c POF4-315
|f POF IV
|x 0
588 _ _ |a Dataset connected to CrossRef, Journals: inrepo02.dkfz.de
700 1 _ |a Stabilini, Alberto
|0 0000-0001-9823-1250
|b 1
700 1 _ |a Thai, Long-Yang Jan
|0 P:(DE-He78)5889f9564a2c825325847329373b61ac
|b 2
|u dkfz
700 1 _ |a Yukihara, Eduardo G.
|b 3
700 1 _ |a Jäkel, Oliver
|0 P:(DE-He78)440a3f62ea9ea5c63375308976fc4c44
|b 4
|u dkfz
700 1 _ |a Vedelago, Jose Alberto
|0 P:(DE-He78)d028533bf57b4053bc9b94b70daab443
|b 5
|e Last author
|u dkfz
773 _ _ |a 10.1016/j.radmeas.2024.107097
|g Vol. 173, p. 107097 -
|0 PERI:(DE-600)2000759-0
|p 107097
|t Radiation measurements
|v 173
|y 2024
|x 1350-4487
856 4 _ |u https://inrepo02.dkfz.de/record/289482/files/1-s2.0-S1350448724000453-main.pdf
856 4 _ |u https://inrepo02.dkfz.de/record/289482/files/1-s2.0-S1350448724000453-main.pdf?subformat=pdfa
|x pdfa
909 C O |o oai:inrepo02.dkfz.de:289482
|p VDB
910 1 _ |a Deutsches Krebsforschungszentrum
|0 I:(DE-588b)2036810-0
|k DKFZ
|b 0
|6 P:(DE-He78)f726c09d369bb3767687f686aa6694fb
910 1 _ |a Deutsches Krebsforschungszentrum
|0 I:(DE-588b)2036810-0
|k DKFZ
|b 2
|6 P:(DE-He78)5889f9564a2c825325847329373b61ac
910 1 _ |a Deutsches Krebsforschungszentrum
|0 I:(DE-588b)2036810-0
|k DKFZ
|b 4
|6 P:(DE-He78)440a3f62ea9ea5c63375308976fc4c44
910 1 _ |a Deutsches Krebsforschungszentrum
|0 I:(DE-588b)2036810-0
|k DKFZ
|b 5
|6 P:(DE-He78)d028533bf57b4053bc9b94b70daab443
913 1 _ |a DE-HGF
|b Gesundheit
|l Krebsforschung
|1 G:(DE-HGF)POF4-310
|0 G:(DE-HGF)POF4-315
|3 G:(DE-HGF)POF4
|2 G:(DE-HGF)POF4-300
|4 G:(DE-HGF)POF
|v Bildgebung und Radioonkologie
|x 0
914 1 _ |y 2024
915 _ _ |a Nationallizenz
|0 StatID:(DE-HGF)0420
|2 StatID
|d 2023-10-22
|w ger
915 _ _ |a JCR
|0 StatID:(DE-HGF)0100
|2 StatID
|b RADIAT MEAS : 2022
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0200
|2 StatID
|b SCOPUS
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0600
|2 StatID
|b Ebsco Academic Search
|d 2023-10-22
915 _ _ |a Peer Review
|0 StatID:(DE-HGF)0030
|2 StatID
|b ASC
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0199
|2 StatID
|b Clarivate Analytics Master Journal List
|d 2023-10-22
915 _ _ |a WoS
|0 StatID:(DE-HGF)0113
|2 StatID
|b Science Citation Index Expanded
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0150
|2 StatID
|b Web of Science Core Collection
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0160
|2 StatID
|b Essential Science Indicators
|d 2023-10-22
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)1150
|2 StatID
|b Current Contents - Physical, Chemical and Earth Sciences
|d 2023-10-22
915 _ _ |a IF < 5
|0 StatID:(DE-HGF)9900
|2 StatID
|d 2023-10-22
920 2 _ |0 I:(DE-He78)E040-20160331
|k E040
|l E040 Med. Physik in der Strahlentherapie
|x 0
920 0 _ |0 I:(DE-He78)E040-20160331
|k E040
|l E040 Med. Physik in der Strahlentherapie
|x 0
920 1 _ |0 I:(DE-He78)E040-20160331
|k E040
|l E040 Med. Physik in der Strahlentherapie
|x 0
980 _ _ |a journal
980 _ _ |a VDB
980 _ _ |a I:(DE-He78)E040-20160331
980 _ _ |a UNRESTRICTED


LibraryCollectionCLSMajorCLSMinorLanguageAuthor
Marc 21