Study of an energy degrader made of B4C/graphite composites

Mean excitation energy determination for Monte Carlo simulations of boron carbide as degrader material for proton therapy

Boron carbide is a material proposed as an alternative to graphite for use as an energy degrader in proton therapy facilities, and is favoured due to its mechanical robustness and promise to give lower lateral scattering for a given energy loss. However, the mean excitation energy of boron carbide has not yet been directly measured. Here we present a simple method to determine the mean excitation energy by comparison with the relative stopping power in a water phantom, and from a comparison between experimental data and simulations we derive a value for it of 83.1 ± 2.8 eV suitable for use in Monte-Carlo simulation. This is consistent with the existing ICRU estimate (84.7 eV with 10-15% uncertainty) that is based on indirect Bragg additivity calculation, but it has a substantially smaller uncertainty. The method described can be readily applied to predict the ionisation loss of other boron carbide materials in which the atomic constituent ratio may vary, and allows this material to be reliably used as an alternative to graphite, diamond or beryllium.

Design of a light and fast energy degrader for a compact superconducting gantry with large momentum acceptance

PURPOSE

Proton therapy is a precise radiation cancer treatment with low side effects. To reduce the cost and footprint of the facility, the superconducting gantry with large momentum acceptance becomes a potential solution. Benefit from this feature, beam delivery time depends largely on the energy-switching process and short time is helpful for increasing the number of volume repaintings.

METHODS

This note introduces an energy degrader with lightweight moving parts and a new hybrid structure (wedge-block-block). The total energies are separated into three stages and are degraded at fixed rates in two boron carbide blocks. As only one pair of graphite wedges is used for energy modulation, the energy switching at each step reaches a 10 ms level.

RESULTS

The transport process in the degrader was simulated in TOPAS. After the degradation, the maximum energy spread (1σ) was approximately 5.5%, and the distance between successive energy layers can be increased for treating non-sensitive tissues. Six configurations of the hybrid degrader achieved distinctly higher transmission efficiencies than the usual graphite multi-wedge degrader. Finally, the configuration that maximized the beam transmission in the lower-energy range (namely, the W-B₁-B₂ configuration) was chosen as the degrader.

CONCLUSIONS

This new degrader not only improved the transmission efficiency, but also reduced the energy-switching time by virtue of its light and compact structure.