Scientific Reports · 2021 · 42 citations · 42 references
MedicineOncologyRadiation OncologyRadiation DosimetryRadiation PhysicsTreatment PlanningAccelerator PhysicsElectron Beam PhysicsExternal Beam RadiotherapyPhantom DosimetryRadiation TherapyStereotactic RadiotherapyBeam Penetration DepthDepth Dose DistributionElectron AcceleratorsElectron Beam FocusingElectron Beam GenerationLaser Wakefield AccelerationPhoton RadiotherapyRadiotherapy Dose Planning
An electron beam of very high energy (50-250 MeV) can potentially produce a more favourable radiotherapy dose distribution compared to a state-of-the-art photon based radiotherapy technique. To produce an electron beam of sufficiently high energy to allow for a long penetration depth (several cm), very large accelerating structures are needed when using conventional radio-frequency technology, which may not be possible due to economical or spatial constraints. In this paper, we show transport and focusing of laser wakefield accelerated electron beams with a maximum energy of 160 MeV using electromagnetic quadrupole magnets in a point-to-point imaging configuration, yielding a spatial uncertainty of less than 0.1 mm, a total charge variation below [Formula: see text] and a focal spot of [Formula: see text]. The electron beam was focused to control the depth dose distribution and to improve the dose conformality inside a phantom of cast acrylic slabs and radiochromic film. The phantom was irradiated from 36 different angles to obtain a dose distribution mimicking a stereotactic radiotherapy treatment, with a peak fractional dose of 2.72 Gy and a total maximum dose of 65 Gy. This was achieved with realistic constraints, including 23 cm of propagation through air before any dose deposition in the phantom.
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T. Tajima, J. M. Dawson · Physical Review Letters · 1979 · 4.6K citations
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J. Fauré, Y. Glinec, A. Pukhov et al. · Nature · 2004 · 2.1K citations
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High-quality electron beams from a laser wakefield accelerator using plasma-channel guiding
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Natural Sciences, Physics, Optics +13