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Synopsis by Brad Thompson
Synopsis by Brad Thompson

... Unfortunately this is one of the two missing equations. Its derivation is easily attainable utilizing the methodology used in the reference. Assuming that the lasing medium is a rod of radius a, the authors propose that, “The laser output energy can then be regarded as proportional to the cross sect ...
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... telecommunications are able to transfer voice and computer images and data with a speed that is one hundred times more than telecommunications networks with copper cables [1]. The process and alteration of optical signals into electric current is troublesome in high speeds, so if the width of optica ...
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... which were first observed by Wood [1] and subsequently subjected to extensive theoretical investigations [2]–[6]. These investigations have been expanded to resonance anomalies in a grating waveguide structure (GWS), and include new theoretical and experimental developments [7]–[16]. The basic GWS i ...
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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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