Fig. 5: Electron beam charge optimization through pulse shaping. | Nature Communications

Fig. 5: Electron beam charge optimization through pulse shaping.

From: Automation and control of laser wakefield accelerators using Bayesian optimization

Fig. 5

a Surrogate model predicted charge on the β(2)β(4) plane at the optimal values of β(3) and f. Markers show the initial position projected onto this plane, A, and the optimal position, B. Marker C shows the likely end result of sequential 1D optimizations of β(2) and β(4) when starting from position A. The diagonal lines show the combination of β(2) and β(4) modifications that maintain an approximately constant pulse shape. b Snapshots from a PIC simulation showing the laser normalized vector potential a, the electron densities of the background plasma and the electrons released from the two inner ionization levels of nitrogen normalized to n0 = 1.2 × 1019 cm−3. c Left: axial laser field envelope at the given z positions and (right) maximum laser field, and total electron beam charge as functions of z position from simulations using the input laser pulse spectral phase coefficients from points A and B from a.

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