Universal and dynamic ridge filter for pencil beam scanning (PBS) proton therapy
Vivek Maradia,
Switzerland
OC-0622
Abstract
Universal and dynamic ridge filter for pencil beam scanning (PBS) proton therapy
Authors: Vivek Maradia1,2, Isabella Colizzi1,2, Anne Savenije1,3, David Meer1, Jacobus Maarten Schippers4, Damien Charles Weber1,5,6, Antony John Lomax1,2, Oxana Actis1, Serena Psoroulas1
1Paul Scherrer Institute, Center for Proton Therapy, Villigen, Switzerland; 2ETH Zurich, Department of Physics, Zurich, Switzerland; 3TU Delft, Department of Physics, Delft, The Netherlands; 4Paul Scherrer Institute, Larger Accelerator facility , Villigen, Switzerland; 5University of Zurich, University Hospital Zurich, Zurich, Switzerland; 6University of Bern, University Hospital Bern, Bern, Switzerland
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Purpose or Objective
Our
objective is to design a universal dynamic energy modulator (ridge filter) for PBS
proton therapy. By using a ridge filter, the Bragg peak is broadened, thus
lowering the number of energies required for homogeneous target coverage.
Treatment delivery time in PBS proton therapy depends on beam-on time and the
dead time (time required to change energy layers and/or lateral position). By
lowering the number of required energies, we want to reduce the treatment
delivery time.
Material and Methods
To
reduce the number of energy layers, we developed a new energy modulation unit
that comprises two identical ridge filters placed just before the isocenter
(shown in Figure 1). Both ridge filters are movable relative to each other to
change the Bragg peak’s characteristics dynamically. For predicting the Bragg
peak shape with the ridge filter, we used Monte Carlo simulations implemented
in TOPAS with the beam model of PSI Gantry 2. To compare the reduction in
energy layers with ridge filter, we generated eight different spread out Bragg
peaks (SOBPs) with a thickness range from 4 to 11 cm with and without the ridge
filter.
Results
Figure
1 shows that a maximum broadening of the Bragg peak is achieved (almost 2 cm
SOBP) if the filter is aligned, peaks with peaks
(figure 1(a)). However, if the filter is aligned peak with valley (figure
1(b)), the ridge filter acts as a range shifter. Figures 1(c) show an 11 cm wide
SOBP generated by the ridge filter while aligning peak with valley for the first
two high-energy beams (to get the sharper fall-off) and for the remaining lower
energies, the filter is aligned in peak-to-peak position (to maximize the Bragg
peak broadening). In this way, the dynamic ridge filter produces a sharper
distal fall-off compared to a normal ridge filter. Table 1 shows the number of
energy layers required to generate different widths of SOBP with and without
ridge filter. With the dynamic ridge filter, we managed to reduce the required
energy layers by a factor of three compared to a SOBP generated without a ridge
filter.
Conclusion
In
this study, we showed that by using a newly developed dynamic ridge filter we
could reduce the number of energy layers required to generate different SOBP by
a factor of three while being independent of energy. As we can use the same ridge filter design
for different types of tumors, the use of a dynamic ridge filter will not
increase the complexity of treatment planning. As this design is not
patient-specific or beam model-specific, it is easily adaptable for other
proton therapy facilities, too.