Ion recombination correction factor in scanned light-ion beams for absolute dose measurement using plane-parallel ionisation chambers

Based on international reference dosimetry protocols for light-ion beams, a correction factor ( k s ) has to be applied to the response of a plane-parallel ionisation chamber, to account for recombination of negative and positive charges in its air cavity before these charges can be collected on the...

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Bibliographic Details
Main Authors: Rossomme, Severine (Author) , Horn, Julian (Author) , Brons, Stephan (Author) , Jäkel, Oliver (Author) , Mairani, Andrea (Author)
Format: Article (Journal)
Language:English
Published: 12 June 2017
In: Physics in medicine and biology
Year: 2017, Volume: 62, Issue: 13, Pages: 5365-5382
ISSN:1361-6560
DOI:10.1088/1361-6560/aa730f
Online Access:Verlag, Volltext: http://dx.doi.org/10.1088/1361-6560/aa730f
Verlag, Volltext: http://stacks.iop.org/0031-9155/62/i=13/a=5365
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Author Notes:S. Rossomme, J. Horn, S. Brons, O. Jäkel, A. Mairani, M. Ciocca, V. Floquet, F. Romano, D. Rodriguez Garcia, S. Vynckier, H. Palmans
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Summary:Based on international reference dosimetry protocols for light-ion beams, a correction factor ( k s ) has to be applied to the response of a plane-parallel ionisation chamber, to account for recombination of negative and positive charges in its air cavity before these charges can be collected on the electrodes. In this work, k s for IBA PPC40 Roos-type chambers is investigated in four scanned light-ion beams (proton, helium, carbon and oxygen). To take into account the high dose-rates used with scanned beams and LET-values, experimental results are compared to a model combining two theories. One theory, developed by Jaffé, describes the variation of k s with the ionization density within the ion track (initial recombination) and the other theory, developed by Boag, describes the variation of k s with the dose rate (volume recombination). Excellent agreement is found between experimental and theoretical k s -values. All results confirm that k s cannot be neglected. The solution to minimise k s is to use the ionisation chamber at high voltage. However, one must be aware that charge multiplication may complicate the interpretation of the measurement. For the chamber tested, it was found that a voltage of 300 V can be used without further complication. As the initial recombination has a logarithmic variation as a function of 1/ V , the two-voltage method is not applicable to these scanned beams.
Item Description:Gesehen am 25.04.2018
Physical Description:Online Resource
ISSN:1361-6560
DOI:10.1088/1361-6560/aa730f