Analysis of various beamlet sizes for IMRT with 6 MV Photons

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Abstract
Application of intensity modulated radiation therapy (IMRT) using multileaf collimation often requires the use of small beamlets to optimize the delivered radiation distribution. Small‐beam dose distribution measurements were compared to dose distributions calculated using a commercial treatment planning system that models its data acquired using measurements from relatively large fields. We wanted to evaluate only the penumbra, percent depth‐dose (PDD) and output model, so we avoided dose distribution features caused by rounded leaf ends and interleaf leakage by making measurements using the secondary collimators. We used a validated radiochromic film dosimetry system to measure high‐resolution dose distributions of 6 MV photon beams. A commercial treatment planning system using the finite size pencil beam (FSPB) dose calculation algorithm was commissioned using measured central axis outputs from 4.0×4.0 to 40.0×40.0 cm2 beams and radiographic‐film profile measurements of a 4.0×4.0 cm2 beam at twice the depth of maximum dose Calculated dose distributions for square fields of 0.5×0.5 cm2, and 1.0×1.0 cm2, to 6.0×6.0 cm2, in 1.0×1.0 cm2, increments were compared against radiochromic film measurements taken with the film oriented parallel to the beam central axis in a water equivalent phantom. The PDD of the smaller field sizes exhibited behavior typical of small fields, namely a decrease in with decreasing field size. The FSPB accurately modeled the depth‐dose and central axis output for depths deeper than the nominal of 1.5 cm plus 0.5 cm. The dose distribution in the build‐up and penumbra regions was not accurately modeled for depths less than 2 cm, especially for the fields of 2.0×2.0 cm2 and smaller. Using the γ function with 2 mm and 2% criteria, the dose model was shown to accurately predict the penumbra. While for single small beams the compared dose distributions passed the γ function criteria, the clinical appropriateness of these criteria is not clear for a composite IMRT plan. Further investigation of the cumulative impact of the observed dose discrepancies is warranted. We speculate that the observed differences in the penumbra regions arise from some energy dependent artifact in the radiographic‐film profiles used for commissioning. In the future, radiochromic film based commissioning might provide a more accurate data set for dose modeling.