Author/Authors :
Yani, S Department of Physics - Faculty of Mathematics and Natural Sciences - IPB University - Bogor 16680, Indonesia , Budiansah, I Department of Physics - Faculty of Mathematics and Natural Sciences - Institut Teknologi Bandung - West Java, 40132, Indonesia , Pratama, S.H Department of Physics - Faculty of Mathematics and Natural Sciences - Institut Teknologi Bandung - West Java, 40132, Indonesia , Rhani, M.F Department of Radiology - Concord International Hospital - Singapore, Singapore , Anam, C Department of Physics - Faculty of Sciences and Mathematics - Diponegoro University, Central Java, Indonesia , Haryanto, F Department of Physics - Faculty of Mathematics and Natural Sciences - Institut Teknologi Bandung - West Java, 40132, Indonesia
Abstract :
Background: The free flattening filter (FFF) beam can affect the characteristics of the linac output such as the maximum dose depth, surface dose, dose in the fall-off area, and doses outside the field because the beam hardening effect does not occur in the FFF linac head. Therefore, the present study
aimed to investigate the influence of the FFF beam on the dose distribution in
an inhomogeneous phantom using the EGSnrc/DOSXYZnrc Monte Carlo
package. Materials and Methods: In the present study, an Elekta Infinity
10 MV photon beam equipped with a multileaf collimator Agility linear
accelerator was used. Two types of virtual inhomogeneous phantoms were
built for percent depth doses (PDDs) and dose profiles measurement. The first
phantom comprised four layers: water (4 cm thickness), bone (2 cm
thickness), lung tissue (5 cm thickness), and water (19 cm thickness). The
second phantom had a half-lung tissue slab and a half-bone slab (10 cm
thickness) on the left side of the water. Results: The PDD curves in the
inhomogeneous phantom considerably decreased in the lung area for small
exposure fields because the charged particle equilibrium was not achieved.
The dose in the lung was higher than the dose in the water when the charged
particle equilibrium was reached. Meanwhile, the dose in the bone is always
lower than the dose in the water. Conclusions: The dose distribution of
flattening filter (FF) and FFF beams in the inhomogeneous phantom was the
same in the small field of exposure. However, differences in dose distribution are increasingly apparent for larger field sizes.
Keywords :
Elekta Infinity , flattening filter free , EGSnrc , heterogeneous phantom