1990
DOI: 10.1088/0031-9155/35/4/004
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An analytic theory of the point-source nonuniformity correction factor for thick-walled ionisation chambers in photon beams

Abstract: In exposure and air kerma measurements, axial and radial nonuniformity perturbation correction factors are used to account for the nonuniformity of the incident photon field in the vicinity of the ionisation chamber cavity. An analytic theory for calculating the point source nonuniformity correction factor for thick-walled ionisation chambers is developed. The theory developed herein is compared with Monte Carlo calculations for chambers with pancake, cylindrical and spherical geometries similar in size to the… Show more

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Cited by 53 publications
(55 citation statements)
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“…Our methodology is applicable to any kind of charged particle, provided that the considered MC code is able to track the charged particle considered. It is a generalization of the regeneration technique of Bielajew 23,24 to all charged particles. One does not need to modify the neutron transport algorithm and the interaction rate (defined by the macroscopic cross section ) can be completely controlled by the user.…”
Section: Resultsmentioning
confidence: 99%
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“…Our methodology is applicable to any kind of charged particle, provided that the considered MC code is able to track the charged particle considered. It is a generalization of the regeneration technique of Bielajew 23,24 to all charged particles. One does not need to modify the neutron transport algorithm and the interaction rate (defined by the macroscopic cross section ) can be completely controlled by the user.…”
Section: Resultsmentioning
confidence: 99%
“…One common method in photon beams is the regeneration technique, introduced by Bielajew. 23,24 In the regeneration technique, the photon keeps its initial momentum and energy at the interaction site, which effectively eliminates photon attenuation and scatter. 5 Secondary electrons are created according to the cross sections.…”
Section: Introductionmentioning
confidence: 99%
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“…Ce facteur correctif est factorisé en deux termes, pour les non-uniformités axiale (k an ) et radiale (k rn ). Le facteur de correction de non-uniformité axiale est pris égal à l'unité [9,10] sans aucune incertitude pour le moment. Le facteur de correction de nonuniformité radiale est déterminé à partir de mesures faites à l'aide d'une petite chambre d'ionisation dans le plan de référence.…”
Section: Corrections De Perturbation Liées Au Détecteurunclassified