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Also the anisotropy function and the radial dose function for this source are graphically compared.
The radial dose function was measured and was found to be similar to that of the silver-based model 6711 125I source.
The radial dose function were presented in graphical format for the comparison between the dose distribution in water and different tissue phantoms.
The dose rate constant, Λ, line and point-source radial dose function, gL r) and gP r), and the anisotropy function, F r,θ) of the IR01-103Pd seed have been calculated at distances from 0.25 to 5 cm.
Measurements are made with LiF thermoluminescent dosimeters (size of 1 mm3) in solid water phantoms WT1 to obtain the dose constant, the radial dose function and the anisotropy function.
It seems that the radial dose function calculated in water differed in tissue phantoms due to the atomic composition and densities for media that are not taken account by the TG43-U1 formalism.
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Radial dose functions were found to depend not only on the phantom size but also on the material density.
The radial dose functions would depend not only on the phantom size but also on the phantom density.
They found that the phantom dimensions significantly affected the radial dose functions near to the edges of the phantom, with deviations of up to 25% being observed.
Tables 1 and 2 also present the radial dose functions and dose-rate constants of bone and lung tissue to provide clinical reference data for dose calculations in various tissue types around an Ir source.
Figure 5 shows the radial dose functions in water near the edge of the phantom, where deviations of up to 23% are evident and the results are similar to those of Karaiskos et al. The deviations in the radial dose functions in bone and lung tissue were 26.7% and 6.5%, respectively.
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