Fig. 3: 6D optimization of betatron X-ray source. | Nature Communications

Fig. 3: 6D optimization of betatron X-ray source.

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

Fig. 3

a Top panel shows the mean (normalized) X-ray yield for each burst (circles) with SE. The dashed line shows the model predicted maximum value of X-ray yield with the shaded region enclosing ±SD uncertainty. The lower panel shows the evolution of the input parameters representing the focal position of the laser pulse (f), the plasma electron density (ne), the plasma source length (Lcell) and three orders of spectral phase (β(2)β(3)β(4)). b X-ray images from the initial and optimal bursts, where the signal for each pixel is the mean from the ten individual shots. The initial X-ray image is multiplied by 5, to make it visible on the same scale. c The projection of the measurements onto each 2D plane of the parameter space, colour coded by the normalized total X-ray counts.

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