Figure 4 | Scientific Reports

Figure 4

From: A tunable electron beam source using trapping of electrons in a density down-ramp in laser wakefield acceleration

Figure 4The alternative text for this image may have been generated using AI.

(a) The green circles correspond to the electron bunch length measurements with beamloading turned off. The green line is a fit using Eq. (3) with C 1 = 0.83 and C 2 = 0. The red plus signs are data points from the simulation of the electron bunch length, the dashed red curve represents a fit according to Eq. (3). The blue crosses and dotted line represents the same values for a gentler gradient slope. (b) Spatial electron density profiles of three different acceleration densities: n 2 = 3, 4 and 5 1018 cm−3. Here, ∂n/∂x = 0.76n 1/λ p1 with beamloading. (c) The peak normalized vector potential a 0 (in blue) and FWHM width (dashed red) as function of the laser pulse’s peak position during a simulation with n 2 = 3 1018 cm−3 and ∂n/∂x = 0.76n 1/λ p1. For the different simulation, the peak value of a 0 varies between 3.8 and 4.3, but the behaviour is the same for all simulations, a 0 increases and the width of the pulse decreases.

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