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Investigation of the relative conformity and efficiency for ... - Wcenter.de

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Conclusions• This study indicates that <strong>the</strong> sensitivity <strong>of</strong> dose <strong>con<strong>for</strong>mity</strong> to beam size <strong>for</strong> IMPT<strong>de</strong>pends on <strong>the</strong> proximity <strong>of</strong> critical structures, <strong>the</strong>ir dose constraints, <strong>and</strong> <strong>the</strong> number<strong>of</strong> beams <strong>de</strong>livered.• With <strong>the</strong> geometrically tight prostate phantom <strong>and</strong> only 2 fields, acceptable resultswere obtained with 3 <strong>and</strong> 6 mm beam σ, but not greater.• With <strong>the</strong> more <strong>for</strong>giving lung phantom geometry, satisfactory results were obtainedwith beam σ up to 12 mm, but only with <strong>the</strong> addition <strong>of</strong> more fields.• Theoretically <strong>the</strong> time difference between 3 <strong>and</strong> 12 mm beam σ <strong>de</strong>livered fields in <strong>the</strong>transverse direction is (3/12)^12=0,0625 a factor <strong>of</strong> 16 times. A longitudinal timedifferential also exists where <strong>the</strong> number <strong>of</strong> energy layers required scales linearly withbeam spot size.• This study suggests that <strong>the</strong>re may be some clinical cases, such as prostate, where<strong>de</strong>livery time may be required to be longer to maintain <strong>con<strong>for</strong>mity</strong>, <strong>and</strong> o<strong>the</strong>rs, suchas lung, where a more efficient <strong>de</strong>livery <strong>of</strong> larger beam spots may be <strong>de</strong>sirable. Thismay also reduce <strong>de</strong>livery sensitivity to target motion.• However, only two limited geometries were consi<strong>de</strong>red <strong>for</strong> this study. Hence, fur<strong>the</strong>rinvestigation is suggested also with clinical cases be<strong>for</strong>e general conclusions can bema<strong>de</strong> regarding suggested beam σ’s <strong>for</strong> IMPT.

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