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eft-handed polarizations having different refractive indices in the material. A linearly polarized wave can be seen as the

sum of two circularly polarized waves with equal amplitude but opposite direction of rotation. As these two waves propagate with different speeds through the material, they will acquire a phase difference proportional to the travelled distance. In terms of their sum, these two beams, when they emerge, have a phase lag between them implying that the emerging beam has a rotated plane of polarization by an angle which is equal to half the phase change. This effect is non..................==> [ Click Here to Read More ]



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