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Role of lattice structure and low temperature resistivity on fast electron beam filamentation in carbon

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Figure 1: (a) Schematic illustrating the experiment arrangement. Lmolecular dynamics simulations coupled with the Kubo-Greenwood approach, as discussed inF and LR correspond to thethickness of the front and rear layers, respectively, in the double layer ta
Figure 2: TOP ROW: Measured proton spatial-intensity dose profiles (Gy) for: (a) LµCorresponding loghybrid-PIC simulations, at 1.2 ps from the start of the electron injection; THIRD ROW: Cor-responding [Y-Z] mid-plane 2D maps of the magnetic flux density (BBOTTOM ROW: Corresponding modelled proton spatial-intensity maps, calculated using the=200µm vitreous carbon; (b) L=200 µm diamond; (c) LF =100 µm vitreous carbon and LR=100m diamond; (d) LF =100 µm diamond and LR=100 µm vitreous carbon; SECOND ROW:10 fast electron density maps (m−3) in the [Y-Z] plane, from 3D Zephyrosx component in Tesla);rear-side fast electron density maps obtained from (e)-(h).
Figure 3: (a) Variation in the rear surface fast electron density in the simulation results (leftaxis) and the measured proton dose (right axis) for the four given target types; (b) Variation inthe fast electron density as a function of the thickness of th
Figure 4: Zephyros simulation results for double layer targets with vitreous carbon as the frontlayer and diamond as the rear
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