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Experimental Study of Proton Acceleration with Ultra-High Intensity, High Contrast Laser Beam

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Academic year: 2021

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Figure 1.3: Evolution of laser power in time.
Figure 3.6: Initial condition for the adiabatic model.
Figure 3.8: Picture of the initial condition for the two cases. In the isothermal case, the density is constant n i (x, t = 0) for x ∈ (−∞, −l ss ] and exponentially decreases on
Figure 3.9: (left) The evolution in time of the accelerating field due to charge separation at the plasma boundary for different initial density gradient lengths
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