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Laser acceleration of protons using multi-ion plasma gaseous targets

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Figure

Figure 1. The initial setup of (a) the laser beam and (b), (c) the particle densities in the target
Figure 2. Two-dimensional density distributions of electrons (1st row) and carbon ions (2nd row), the carbon ion phase space (3rdrow), and the one-dimensional density distribution (4th row) of electrons, carbon ions, and their differences, which are plotted byaveraging over−0.5λ<y<0.5λLL ,at times =t20TL, 40TL, 70TL, 120TLand 180TL.
Figure 4. The phase space (1st row), two-dimensional density distribution (2nd row), and one-dimensional density distribution (3rdrow) of protons, plotted by averaging over−0.5λ<y<0.5λLL ,at times =t20TL, 40TL, 70TL, 120TLand 180TL.
Figure 7. The one-dimensional density distributions (thedensity first two columns) and energy spectra (the last two columns) of protonswithin∣ ∣ <yλL at =t150T L and =t300T L between the original case ofn=e0 max10ncr (the 1st row) and the case with doubled peakn=e0 max20ncr (the 2nd row).
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