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The degree of polarization may depend on the angle of reflection and the polarized light reflected by the beetles may have function in recognition of the species.
When a ray of light is reflected at a polished surface, the angle of reflection between ray and normal (the line at right angles to the surface) is exactly equal to the angle of incidence.
Thus, multiple diffraction produces a reflected beam at a wavelength longer than the angle of reflection and the spacing of the horizontal planes should allow when Bragg's law is applied to them.
Hence, the angle of incidence can be assumed to be equal to the angle of reflection.
The specular component has the angle of incidence w.r.t to normal n 1 equal to the angle of reflection, θ.
Concretely, we check, for each reflection point, if the angle of reflection θr equals the angle of incidence θ i, as shown in Figure 3.
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Naturally, the reflection factor is changed according to the shape of obstacles, the angle of reflections, and so on.
It is natural that the reflection factor is changed according to the matter of the obstacles, the angle of reflections and so on.
According to the generalized Snell's law the angles of reflection θ r and refraction θ t are related to the incidence angle θ i by the generalized Snell's law, (sin theta _{i}+{{1} over {k_{0}}}{{dPhi } over {dx}}=sin theta _{t}=sin theta _{r}) [15].
When the reflection coefficients of s- and p-polarized radiation have equal amplitude values, i.e., R s 2 = R p 2, and the magnitude of polarization difference ρ equals zero, the light reflection occurs regardless of polarization state at the angle of isotropic reflection θρ = 0 [32].
When the reflection coefficients of s- and p-polarized radiation have equal amplitude values, i.e. r s 2 = r p 2, and the magnitude of polarization difference ρ equals zero, the light reflection occurs regardless of polarization state at the angle of isotropic reflection θ ρ=0 [36].
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