Open AccessDosimetric dependence of the dimensional characteristics on a lead shield in electron radiotherapy: a Monte Carlo study
Author(s) -
Chow James C L,
Grigorov Grigor N
Publication year - 2009
Publication title -
journal of applied clinical medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.83
H-Index - 48
ISSN - 1526-9914
DOI - 10.1120/jacmp.v10i2.2918
Subject(s) - monte carlo method , imaging phantom , materials science , cathode ray , electron , beam (structure) , half value layer , electromagnetic shielding , attenuation , percentage depth dose curve , physics , atomic physics , optics , ionization chamber , nuclear physics , mean free path , composite material , ionization , ion , statistics , mathematics , quantum mechanics
This study investigates the dosimetric dependence of the dimension of a lead (Pb) layer for shielding using clinical electron beams with different energies. Monte Carlo simulations were used to generate phase space files for the 4, 9 and 16 MeV electron beams produced by a Varian 21 EX linear accelerator using the EGSnrc‐based BEAMnrc code, and validated by measurements using films. Pb layers with different thicknesses (2, 4, 6 and 8 mm) and diameters (2.5, 3, 3.5 and 4 cm) were placed at the center of an electron field on a solid water phantom. Beam profiles were determined at the depth of maximum dose ( d m ) using Monte Carlo simulations. The dose profiles under the Pb layer atd m, including the penumbra at the edge of the layer and relative dose at the central beam axis (CAX), were studied with varying thicknesses and diameters of Pb. It is found that 2 mm of Pb is adequate to provide 5 half value layer (HVL) attenuation for the 4 MeV electron beams, and the beam profiles atd mare dependent on the diameter but not the thickness of the Pb. However, for the 9 and 16 MeV electron beams, the relative dose at the CAX andd mdepends on both the thickness and diameter of the Pb layer. For 8 mm thickness of Pb, 4 and 5 HVL attenuation of electron beams with energies of 9 and 16 MeV can be achieved atd m, respectively. Moreover, the beam profile under the Pb layer atd mdepends on: (1) the penumbra region at the edge of the Pb layer; (2) the beam attenuation varying with the thickness of the Pb layer; (3) the electron side scatter contributing to the CAX under the Pb layer; and (4) the photon contamination produced by the Pb layer. A parameter called “shielding area factor” (defined as the ratio of the length between two points of 50% relative doses in the beam profile atd mto the diameter of the Pb layer) is suggested to predict the required size and thickness of Pb for shielding a target with known dimension atd m. The dosimetric data calculated by Monte Carlo simulations in this study are useful to select the suitable thickness and size of Pb for the protection of critical tissue in electron radiotherapy. PACS number: 87.53.Bn; 87.55.kh and 87.55.km.