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Role of magnetic field evolution on filamentary structure formation in intense laser-foil interactions

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Figure

Figure 1.(a) Schematic illustrating of the relevant aspects of thetarget normal. The spatial profile and energy of the beam of acceleratedprotons are measured using a radiochromic film stack at the rear of thetarget
Figure 2. Example proton spatial-intensity profile at 2.2 MeV for (a)E10 nm Al target. The dashed insets show a magnified region, highlightingthe filamentary structures
Figure 3. 2D simulation results at(b) the electron density,from the left along thewhen the peak of the first pulse reaches the target) for a laser pulse with0 t = −0.325 ps (where t = 0 is the time E1 =.1E0 showing the spatial profile of (a) the transverse m
Figure 4ments for thea larger simulation was conducted as previously defined inorder to prevent the protons from leaving the simulation box.The filaments maintain their structure fromtthis can modify the detail of the structures formed in theproton beam, we
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