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Fig. 6 Transverse cross-sections of the vessel-filtered TOF-MRA data as a function of sphere radius in mm.
Nietiadi et al. carried out an extensive simulation study of the sputter yield as a function of sphere radius R [14, 15], using both Monte Carlo and exemplary MD simulations.
The original unfiltered TOF-MRA data and the result from the multiscale combination (Eq. 4) is also shown Fig. 7 Coronal maximum intensity projections of the vessel-filtered TOF-MRA data as a function of sphere radius in millimeters.
They showed that sputtering has a maximum as a function of sphere size when the ion penetration depth is of the order of the sphere radius; these results corroborate the earlier findings of Järvi et al. [12, 13].
However, it is worth noting that the minimum RMSE was below 0.12 for each harmonized setting (Fig. 3) and that the harmonized SUV curves as a function of sphere size are close to the curve of DRO17 mm as shown in Fig. 4.
The 'recovery coefficient' is finally defined as a function of sphere size and VOI definition.
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A range of factors that in theory could affect accuracy of the simulation results are examined, including edge roundedness, surface roughness and restitutional behaviour as a function of sphere-composite representations.
Fig. 5 a e Recovery coefficients as a function of hot sphere size from five different hot sphere activity concentrations across all sites.
Fig. 6 a e Recovery coefficients as a function of hot sphere size from three consecutive scans at a single site.
(c) Enhancement due to two-dimensional array of Ag spheres on InGaN/GaN QW emitters with a separation of 10 nm as a function of the sphere radius a for different original radiative efficiencies.
(b) Enhancement due to isolated Ag spheres on InGaN/GaN QW emitters with a separation of 10 nm as a function of the sphere radius a for different original radiative efficiencies.
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