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1.
Med Phys ; 32(8): 2455-63, 2005 Aug.
Article in English | MEDLINE | ID: mdl-16193774

ABSTRACT

We present EGS4 Monte Carlo calculations of the spatial distribution of the dose deposited by a single x-ray pencil beam, a planar microbeam, and an array of parallel planar microbeams as used in radiation therapy research. The profiles of the absorbed dose distribution in a phantom, including the peak-to-valley ratio of the dose distribution from microbeam arrays, were calculated at micrometer resolution. We determined the dependence of the findings on the main parameters of photon and electron transport. The results illustrate the dependence of the electron range and the deposited in-beam dose on the cut-off energy, of the electron transport, as well as the effects on the dose profiles of the beam energy, the array size, and the beam spacing. The effect of beam polarization also was studied for a single pencil beam and for an array of parallel planar microbeams. The results show that although the polarization effect on the dose distribution from a 3 cm x 3 cm microbeam array inside a water phantom is large enough to be measured at the outer side of the array (16% difference of the deposited dose for x-ray beams of 200 keV), it is not detectable at the array's center, thus being irrelevant for the radiation therapy purposes. Finally we show that to properly compare the dose profiles determined with a metal oxide semiconductor field emission transistor detector with the computational method predictions, it is important to simulate adequately the size and the material of the device's Si active element.


Subject(s)
Models, Biological , Radiometry/methods , Radiotherapy Planning, Computer-Assisted/methods , Software , Body Burden , Computer Simulation , Models, Statistical , Monte Carlo Method , Radiotherapy Dosage , Relative Biological Effectiveness , Scattering, Radiation , X-Ray Therapy/methods , X-Rays
2.
Med Phys ; 28(9): 1931-6, 2001 Sep.
Article in English | MEDLINE | ID: mdl-11585224

ABSTRACT

A bent Laue monochromator and a conventional x-ray tube were used to produce a fan beam that was parallel in the plane perpendicular to the plane of the fan. The x-ray fan beam was tunable in energy and had about 12% energy bandwidth at a slice height of 5 mm when tuned to 50 keV. The beam's energy was slightly coupled to the vertical position on the beam's height. The slice height could be varied from 1 to 10 mm. The flux at 50 keV was approximately 2x10(6) photons/mm2/s with a rotating anode tungsten x-ray tube operating at 120 kVp and 100 mA. The narrow energy bandwidth of the beam produced is advantageous over a conventional divergent polychromatic beam for all radiography applications, while the parallelism of the beam enhances its intensity by about threefold and offers some advantages for computed tomography.


Subject(s)
Tomography, X-Ray Computed/instrumentation , Biophysical Phenomena , Biophysics , Equipment Design , Models, Theoretical , Optics and Photonics/instrumentation , Tomography, X-Ray Computed/statistics & numerical data , X-Rays
3.
Cell Mol Biol (Noisy-le-grand) ; 47(3): 485-93, 2001 May.
Article in English | MEDLINE | ID: mdl-11441956

ABSTRACT

Duck embryo was studied as a model for assessing the effects of microbeam radiation therapy (MRT) on the human infant brain. Because of the high risk of radiation-induced disruption of the developmental process in the immature brain, conventional wide-beam radiotherapy of brain tumors is seldom carried out in infants under the age of three. Other types of treatment for pediatric brain tumors are frequently ineffective. Recent findings from studies in Grenoble on the brain of suckling rats indicate that MRT could be of benefit for the treatment of early childhood tumors. In our studies, duck embryos were irradiated at 3-4 days prior to hatching. Irradiation was carried out using a single exposure of synchrotron-generated X-rays, either in the form of parallel microplanar beams (microbeams), or as non-segmented broad beam. The individual microplanar beams had a width of 27 microm and height of 11 mm, and a center-to-center spacing of 100 microm. Doses to the exposed areas of embryo brain were 40, 80, 160 and 450 Gy (in-slice dose) for the microbeam, and 6, 12 and 18 Gy for the broad beam. The biological end point employed in the study was ataxia. This neurological symptom of radiation damage to the brain developed within 75 days of hatching. Histopathological analysis of brain tissue did not reveal any radiation induced lesions for microbeam doses of 40-160 Gy (in-slice), although some incidences of ataxia were observed in that dose group. However, severe brain lesions did occur in animals in the 450 Gy microbeam dose groups, and mild lesions in the 18 Gy broad beam dose group. These results indicate that embryonic duck brain has an appreciably higher tolerance to the microbeam modality, as compared to the broad beam modality. When the microbeam dose was normalized to the full volume of the irradiated tissue. i.e., the dose averaged over microbeams and the space between the microbeams, brain tolerance was estimated to be about three times higher to microbeam irradiation as compared with broad beam irradiation.


Subject(s)
Brain/embryology , Brain/radiation effects , Ducks , Radiation Injuries/embryology , X-Ray Therapy/adverse effects , Animals , Ataxia/physiopathology , Body Weight/radiation effects , Brain/pathology , Dose-Response Relationship, Radiation , Ducks/embryology , Models, Animal , Monte Carlo Method , Radiation Dosage , Radiation Injuries/pathology , Radiation Injuries/physiopathology , Survival Rate , Synchrotrons , Time Factors
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