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. 2017 Dec 15;6(12):e17112. doi: 10.1038/lsa.2017.112

Figure 5.

Figure 5

The ripple period, Λ, vs plasma density Ne calculated for different pulse energies and number of the overlapping pulses per spot, N. Theoretical curves are plotted for different ZnS fractions, (1−x), of an effective surface permittivity to account for surface ripple formation and the corresponding change the surface reflectivity; x is the fraction of air.