2011
DOI: 10.1118/1.3560459
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Dose response of alanine detectors irradiated with carbon ion beams

Abstract: The used model and its implementation show a good overall agreement for quasi-monoenergetic measurements. Deviations in depth-dose measurements are mainly attributed to uncertainties of the detector geometry implemented in the Monte Carlo simulations.

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Cited by 23 publications
(14 citation statements)
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“…However, when the particles hit this block, they are displaced along the z axis corresponding to the varying thickness of the ripple structure. In this paper the performance of the ripple filter is tested against an experimental depth-dose curve set (Herrmann et al 2011) acquired at the Schwerionensynchrotron accelerator at Gesellschaft für Schwerionenforschung (GSI), Darmstadt, Germany. In the experiment, a depth-dose curve was measured for a 2  2 cm 270.55MeV/u C12 beam in a water phantom with a Markus ionization chamber by PTW, Freiburg, Germany, using a 3 mm polymethyl methacrylate (PMMA) ripple filter described in Weber and Kraft (1999).…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…However, when the particles hit this block, they are displaced along the z axis corresponding to the varying thickness of the ripple structure. In this paper the performance of the ripple filter is tested against an experimental depth-dose curve set (Herrmann et al 2011) acquired at the Schwerionensynchrotron accelerator at Gesellschaft für Schwerionenforschung (GSI), Darmstadt, Germany. In the experiment, a depth-dose curve was measured for a 2  2 cm 270.55MeV/u C12 beam in a water phantom with a Markus ionization chamber by PTW, Freiburg, Germany, using a 3 mm polymethyl methacrylate (PMMA) ripple filter described in Weber and Kraft (1999).…”
Section: Methodsmentioning
confidence: 99%
“…Figure 1 shows the total dose from a SHIELD-HIT10A simulation of a 270.55 MeV/u 12 C beam, widened with a 3 mm ripple filter. This is compared with an experimental depth-dose curve acquired at GSI (Herrmann et al 2011), as described Figure 1. Absolute depth-dose curve from a 270.55 MeV/u 12 C beam in water (r  1 g/cm 3 ), measured in a cylinder with a radius of 2.65 mm in slices of 0.1 mm.…”
Section: Modifications Of the Physical Modelsmentioning
confidence: 99%
“…The EPR dosimetric method has many advantages such as simple and rapid dose evaluation, the readout procedure is non-destructive, linear response of many organic and inorganic compounds (Regulla, 2005;Ciesielski et al, 2011;Gustafsson et al, 2005;Wieser, 2012;Longo et al, 2010;Fattibene et al, 2011Fattibene et al, , 2014Lund et al, 2002;Guidelli and Baffa, 2014;Parlato et al, 2007;Marrale et al, 2007aMarrale et al, ,b, 2008bMarrale et al, , 2009bMarrale et al, ,a, 2011bMarrale et al, ,c,a, 2012bMarrale et al, , 2014d2013a). EPR detectors show a behavior that suggests possible applications for various kinds of beams used for radiation therapy (Herrmann et al, 2011). Nowadays, the most widely used organic compound as a dosimeter is the alanine (Baffa and Kinoshita, 2014;Marrale et al, 2007aMarrale et al, ,b, 2008bTrompier et al, 2009).…”
Section: Introductionmentioning
confidence: 97%
“…These features allowed alanine to be classified as a reference standard dosimetry system by the IAEA for the measurement of high doses [22]. EPR detectors show a behavior that suggest a possible extension of their use also in hadrontherapy with protons, carbon ions [23,24] and neutrons [17,19,[25][26][27][28][29][30][31]. Alanine/EPR dosimetry is suitable for IORT dosimetry because alanine response has found to be independent of the dose rate even for the high dose rates used in this radiotherapeutic technique [7].…”
Section: Introductionmentioning
confidence: 98%