Experimental determination of wall correction factors. Part II: NACP and Markus plane-parallel ionization chambers
F.W. Wittkämper, A.H.L. Aalbers, B.J. Mijnheer
Abstract
Open-access reader
F.W. Wittkämper, A.H.L. Aalbers, B.J. Mijnheer
Abstract
Open-access reader
For pt.I see ibid., vol.35, p.835-46 (1990). The formalism to derive the absorbed dose to water from ionization chamber measurements in a phantom includes several wall correction factors, k att , k m and p wall , that depend on the shape, size and composition of the ionization chamber. Wall correction factors have been measured for a number of NACP and PTW/Markus chambers. Significant deviations from calculated values occur due to uncertainties in the contribution to the total ionization from the different materials of these inhomogeneous ionization chambers. Experimental values of p wall larger than one have been obtained for the NACP chamber indicating that the side and back wall material of this chamber reduce the ionization compared with the situation where all electrons originate from the water phantom.
OpenAlex reports 21 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
For pt.I see ibid., vol.35, p.835-46 (1990). The formalism to derive the absorbed dose to water from ionization chamber measurements in a phantom includes several wall correction factors, k att , k m and p wall , that depend on the shape, size and composition of the ionization chamber. Wall correction factors have been measured for a number of NACP and PTW/Markus chambers. Significant deviations from calculated values occur due to uncertainties in the contribution to the total ionization from the different materials of these inhomogeneous ionization chambers. Experimental values of p wall larger than one have been obtained for the NACP chamber indicating that the side and back wall material of this chamber reduce the ionization compared with the situation where all electrons originate from the water phantom.
Key concepts: Ionization, Ionization chamber, Imaging phantom, Electron, Atomic physics, Formalism (music), Materials science, Physics