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

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Results• The results from <strong>the</strong> prostate phantom plan QI scores are reported in <strong>the</strong>Table below.• The prostate phantom QI’s indicated a significant sensitivity to beam size.• For <strong>the</strong> prostate case a low QI was only achieved by <strong>the</strong> 3 <strong>and</strong> 6 mm σbeams.• This result is supported by <strong>the</strong> target <strong>and</strong> rectal DVH’s that indicate similaritybetween <strong>the</strong> 3 <strong>and</strong> 6 mm σ beams, but compromise with larger beams.Con<strong>for</strong>mity OAR Hit QIProstate Phantom3mm - 2 Field 1 1.0 16mm - 2 Field 2 1.1 29mm - 2 Field 5 1.1 512mm - 2 Field 17 1.2 14Highly con<strong>for</strong>mal 3 mm σ 2 field plan result1293,61293,6% dose difference between 3 mm <strong>and</strong> 12 mm σplans indicating excess dose to <strong>the</strong> simulatedrectal structure


Results• The results from <strong>the</strong> lung phantom plan QI scores are reported in <strong>the</strong> Tablebelow.• Beam σ from 3-12 mm were capable <strong>of</strong> providing QI scores between 1-3.• However, to achieve this result, a higher total number <strong>of</strong> beams wererequired as sigma increased.• Because 2-3 proton beams are commonly used in clinical lung treatments,<strong>the</strong>re<strong>for</strong>e this was not consi<strong>de</strong>red to be problematic.Lung Phantom Con<strong>for</strong>mity OAR Hit QI3mm - 1 Field 1 1.0 16mm - 1 Field 2 1.3 26mm - 2 Field 1 1.0 19mm - 1 Field 4 1.6 29mm - 2 Field 3 1.1 29mm - 3 Field 2 1.1 212mm - 1 Field 7 1.7 412mm - 2 Field 5 1.2 512mm - 3 Field 5 1.4 3Right: Axial dose difference<strong>of</strong> single 3 <strong>and</strong> 12 mm σbeams surrounding target(interior dashed line).Right: 2 fields <strong>of</strong>6 mm σ<strong>de</strong>livered to aspherical target(gray) within anorgan at risk(green)


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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