Abstract

In proton minibeam radiation therapy, proton minibeams are typically produced by modulating a uniform field using a multislit collimator. Multislit collimators produce minibeams of fixed length and width, and a new collimator has to be manufactured each time a new minibeam array is required, limiting its flexibility. In this work, we propose a scanning dynamic collimator for the generation of proton minibeams arrays. The new collimator system proposed is able to produce any minibeam required on an on-line basis by modulating the pencil beam spots of modern proton therapy machines, rather than a uniform field. The new collimator is evaluated through Monte Carlo simulations and the produced proton minibeams are compared with that of a multislit collimator. Furthermore, a proof of concept experiment is conducted to demonstrate the feasibility of producing a minibeam array by repositioning (i.e. scanning) a collimator. It is concluded that besides the technical challenges, the new collimator design is producing equivalent minibeam arrays to the multislit collimator, whilst is flexible to produce any minibeam array desired.

Highlights

  • In proton minibeam radiation therapy, proton minibeams are typically produced by modulating a uniform field using a multislit collimator

  • Contrary to conventional proton therapy, Proton Minibeam radiation therapy (pMBRT) uses multiple coulomb scatting to its advantage: proton minibeams get increasingly wider as a function of depth, which may result in a homogeneous target dose c­ overage[1], while normal tissues at the entrance will benefit from the spatial fractionation of the dose

  • The new collimator design introduces the concept of a scanning dynamic collimator for the production of a minibeam array

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Summary

Introduction

In proton minibeam radiation therapy, proton minibeams are typically produced by modulating a uniform field using a multislit collimator. The new collimator system proposed is able to produce any minibeam required on an on-line basis by modulating the pencil beam spots of modern proton therapy machines, rather than a uniform field. The generation method influences the shape and size of minibeams, the peak-to-valley dose ratio (PVDR) but as well potential neutron ­contamination[11,12]. All of these aspects have an impact on the biology r­ esponse[4]. The main advantage of minibeam generation with multislit collimators is that it enables its implementation at any proton therapy c­ entre[15]. The main drawbacks are their inefficiency, inflexibility (a custom collimator may have to be fabricated for each case) and introduce a source of secondary neutrons close to the ­patient[12,16]

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