https://orcid.org/0009-0002-8332-9655
Figures & data
Figure 1. Impact of the thickness (left), GT (Middle), and geometrical CTC (right) on the actual throughput generated by tungsten MSC of 30 mm thickness.
Figure 2. (a) Energy spectra of proton beam before and after a collimator. The number of protons is normalised to the peak value of the maximum energy layer. Panel (b) and (c) show depth-dose curves (at peak and valley) with and without collimator, non-optimised, and optimised for homogenous dose in the PTV for the in vivo setup described in Overgaard et al. [Citation12].
![Figure 2. (a) Energy spectra of proton beam before and after a collimator. The number of protons is normalised to the peak value of the maximum energy layer. Panel (b) and (c) show depth-dose curves (at peak and valley) with and without collimator, non-optimised, and optimised for homogenous dose in the PTV for the in vivo setup described in Overgaard et al. [Citation12].](/cms/asset/b20687d3-36cb-4182-9c82-b341c1860f0e/ionc_a_2266125_f0002_c.jpg)
Table 1. Simulated data for a water phantom starting at the iso-center plane (z = 0), and the edge of the MSC facing the iso center positioned at z = −30 mm.
Data availability statement
The datasets used and/or analysed during this study are available from the corresponding author upon reasonable request.