Monte Carlo Simulations Of The Dose Distributions From Carbon Microbeams Used In An Experimental Radiation Therapy Method

被引:1
|
作者
Dioszegi, I. [1 ]
Rusek, A. [2 ]
Dane, B. R. [3 ]
Chiang, I. H. [2 ]
Meek, A. G. [4 ]
Dilmanian, F. A. [4 ,5 ]
机构
[1] Brookhaven Natl Lab, Nonproliferat & Natl Secur Dept, Upton, NY 11973 USA
[2] NASA, Brookhaven Natl Lab, Space Radiat Lab, Upton, NY 11973 USA
[3] SUNY Stony Brook, Sch Med, Stony Brook, NY 11794 USA
[4] SUNY Stony Brook, Dept Radiat Oncol, Stony Brook, NY 11794 USA
[5] Brookhaven Natl Lab, Med Dept, Upton, NY 11973 USA
关键词
Monte Carlo simulation; MCNPX; Carbon radiotherapy; microbeam; ION RADIOTHERAPY; BEAM;
D O I
10.1063/1.3586130
中图分类号
O59 [应用物理学];
学科分类号
摘要
Recent upgrades of the MCNPX Monte Carlo code include transport of heavy ions. We employed the new code to simulate the energy and dose distributions produced by carbon beams in rabbit's head in and around a brain tumor. The work was within our experimental technique of interlaced carbon microbeams, which uses two 90 degrees arrays of parallel, thin planes of carbon beams (microbeams) interlacing to produce a solid beam at the target. A similar version of the method was earlier developed with synchrotron-generated x-ray microbeams. We first simulated the Bragg peak in high density polyethylene and other materials, where we could compare the calculated carbon energy deposition to the measured data produced at the NASA Space Radiation Laboratory (NSRL) at Brookhaven National Laboratory (BNL). The results showed that new MCNPX code gives a reasonable account of the carbon beam's dose up to similar to 200 MeV/nucleon beam energy. At higher energies, which were not relevant to our project, the model failed to reproduce the Bragg-peak's extent of increasing nuclear breakup tail. In our model calculations we determined the dose distribution along the beam path, including the angular straggling of the microbeams, and used the data for determining the optimal values of beam spacing in the array for producing adequate beam interlacing at the target. We also determined, for the purpose of Bragg-peak spreading at the target, the relative beam intensities of the consecutive exposures with stepwise lower beam energies, and simulated the resulting dose distribution in the spread out Bragg-peak. The details of the simulation methods used and the results obtained are presented.
引用
收藏
页码:406 / 409
页数:4
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