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Diffraction grating has periodic structure that splits and diffracts light
Diffraction grating has periodic structure that splits and diffracts light

... be used to demonstrate the effect by reflecting sunlight off them onto a white wall. (see ). This is a side effect of their manufacture, as one surface of a CD has many small pits in the plastic, arranged in a spiral; that surface has a thin layer of metal applied to make the pits more visible. The ...
Properties of different LC cells with high optical anisotropy as a
Properties of different LC cells with high optical anisotropy as a

... Properties of different LC cells with high optical anisotropy as a dynamic holographic media The diffraction efficiency in characteristic nematic range temperatures was measured in DTWM built inside a temperature chamber. That chamber allowed the environmental temperature range to be changed from – ...
Parametric solitons in isotropic media.
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... b) the energy of each component – at every moment of the interaction, even in the case when the components could be separated on different pieces, the localized energy is constant ...
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... diffracted and transmitted beam wave-vectors in off-Bragg incidence. The first functional form is from the Kogelnik’s CWT: jqj = b and r = q  K (Eq. (1)), which assumes efficient phase-matching but allows for jrj 5 b. The second relation is our correction to the CWT: qn = q + n and rn = q  K + n (Eq. ( ...
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Evanescent-field optical microscopy: effects of polarization, tip

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micro-bending, macro-bending and less bend sensitive optical

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Birefringence



Birefringence is the optical property of a material having a refractive index that depends on the polarization and propagation direction of light. These optically anisotropic materials are said to be birefringent (or birefractive). The birefringence is often quantified as the maximum difference between refractive indices exhibited by the material. Crystals with asymmetric crystal structures are often birefringent, as are plastics under mechanical stress.Birefringence is responsible for the phenomenon of double refraction whereby a ray of light, when incident upon a birefringent material, is split by polarization into two rays taking slightly different paths. This effect was first described by the Danish scientist Rasmus Bartholin in 1669, who observed it in calcite, a crystal having one of the strongest birefringences. However it was not until the 19th century that Augustin-Jean Fresnel described the phenomenon in terms of polarization, understanding light as a wave with field components in transverse polarizations (perpendicular to the direction of the wave vector).
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