Notes. For a CH density of ρ_CH = 0.1, the Brewster angle, θ_B, is equal to 72.5°, the phase inversion angle, θ_P, is equal to 70.8°, and the critical angle, θ_C, is equal to 71.6°. One can see that incident angles above the Critical angle lead to transmitted waves whereas incident angles below the Critical angle result in pure reflection. The Brewster angle θ_B represents a situation of perfect transmission, and the Phase inversion angle θ_P separates enhanced from depleted reflection. For linear waves this implies that an enhanced incoming wave with an incident angle between the Brewster angle and the Phase inversion angle gets reflected as an enhanced wave, whereas incoming waves that exhibit an incident angle outside of this range undergo a phase change and propagate as depleted reflections.