Medical Physics · 1986 · 290 citations · 0 references
MedicineRadiation OncologyRadiation DosimetryRadiation PhysicsRadiation TransportAbsorbed DoseMonte Carlo DosimetryMonte Carlo Radiation TransportPhoton DosimetryThree-dimensional Dose DistributionTreatment Planning PhysicsAngular Distribution Of RadiationCollision DensityDose Distribution CalculationsMonte Carlo Dose ModelingMonte Carlo Dose SimulationPencil Beam DosimetryPhoton Dose CalculationPhoton Dose Distribution
Differential pencil beam (DPB) dose is defined as the dose distribution relative to the first collision per unit collision density for a monoenergetic photon pencil beam in an infinite homogeneous medium, and its 3‑D transport of photons and electrons is automatically incorporated. The study aims to predict dose distributions near beam boundaries and blocks by utilizing the angular distribution of incident photons. Dose is computed by evaluating 3D integrals of DPB dose, with calculations performed using energy spectra generated by Monte Carlo, and inhomogeneities are accounted for by attenuating primary fluence, scaling by attenuation coefficients, and adjusting path lengths with effective density. DPB dose distribution tables for various photon energies in water were generated via Monte Carlo, and the DPB model was applied to calculate dose distributions for 6 MV Co and accelerator beams.
Differential pencil beam (DPB) is defined as the dose distribution relative to the position of the first collision, per unit collision density, for a monoenergetic pencil beam of photons in an infinite homogeneous medium of unit density. We have generated DPB dose distribution tables for a number of photon energies in water using the Monte Carlo method. The three‐dimensional (3D) nature of the transport of photons and electrons is automatically incorporated in DPB dose distributions. Dose is computed by evaluating 3D integrals of DPB dose. The DPB dose computation model has been applied to calculate dose distributions for 6 0 Co and accelerator beams. Calculations for the latter are performed using energy spectra generated with the Monte Carlo program. To predict dose distributions near the beam boundaries defined by the collimation system as well as blocks, we utilize the angular distribution of incident photons. Inhomogeneities are taken into account (1) by attenuating the primary photon fluence exponentially utilizing the average total linear attenuation coefficient of intervening tissue, (2) by multiplying photon fluence by the linear attenuation coefficient to yield the number of collisions in the scattering volume, and (3) by scaling the path between the scattering volume element and the computation point by an effective density.