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This formula generalizes the one in the previous section for homogeneous media and includes both waveguide dispersion and material dispersion. The reason for defining the dispersion in this way is that | D | is the (asymptotic) temporal pulse spreading Δ t per unit bandwidth Δ λ per unit distance travelled, commonly reported in ps /( nm ⋅ ...
Improved versions of the prism sheet have a wavy rather than a prismatic structure, and introduce waves laterally into the structure of the sheet while also varying the height of the waves, directing even more light towards the screen and reducing aliasing or moiré between the structure of the prism sheet and the subpixels of the LCD.