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Fig. 6 2D FDTD models of surface scratches: (a) semi-oval/elliptical scratch and (b) semi-diamond/triangular scratch Fig. 7 Electric field distributions inside KDP crystal around (a) elliptical scratch and (b) triangular scratch.
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a elliptical scratches of different width and depth; (b) triangular scratches of different width and depth.
For instance, for 1.0 μm deep, 8 μm wide scratches, the light enhancement can be 2.93 times incident light for elliptical scratches and 2.05 times for triangular scratches.
The light enhancement is increased from 1.24 to 1.98 and 1.99 for triangular scratches with cracks and from 1.6 to 2.55 and 2.56 for elliptical scratches.
The enhancement of light intensity by elliptical scratches seems more remarkable when the depth and width of elliptical and triangular scratches are similar.
When width-depth ratio is less than 5 for 10 μm wide scratch, maximal light enhancement caused by triangular scratches is more pronounced than elliptical ones.
Fig. 9 Maximal light enhancement with respect to width of scratches for elliptical and triangular scratches with the width-to-depth ratios of (a) 2 and (b) 20.
Fig. 10 Maximal light enhancement with respect to width-to-depth ratio for elliptical and triangular scratches of (a) 2 μm and (b) 10 μm wide.
For both elliptical and triangular scratches, the maximal light intensity due to scratches increases with the depth of the scratches and decreasing the width will also result in the enhancement of light intensity.
The light enhancement is nearly linearly proportional to the width of scratches while it is almost unchanged for triangular scratches when the width of scratches exceeds 3 μm in the modeled situations.
The triangular cross-sectioned scratch S8 is damaged at 10.78 J/cm2 similar to that S9 slid by spherical indenter 10.97 J/cm2.
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