Abstract
Physical interpretations of optical activity ultimately derive from the general helix model introduced by Fresnel (1824) to account for optical rotation in terms of the then newly-developed transverse vibration theory of light. The discovery of the left-circular and right-circular polarization modes of radiation by Fresnel, through the introduction of the quarter-wave plate, the Fresnel rhomb, and the triprism composed of (+)- and (-)-quartz elements, enabled him to ascribe optical rotation to a circular birefringence of the active medium. Plane-polarized radiation, regarded as the resultant of superposed left and right circularly polarized components with equal amplitudes, undergoes a rotation if one component is retarded relative to the other on propagation through a transparent medium. The angle of rotation in radians, (ϕ, at the wavelength, λ, for a unit path-length is given by the Fresnel equation,
where nL and nR are the refractive index of the medium for left and right circularly polarized light, respectively [1].
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Mason, S.F. (1979). General Models for Optical Activity. In: Mason, S.F. (eds) Optical Activity and Chiral Discrimination. NATO Advanced Study Institutes Series, vol 48. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-7644-4_1
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DOI: https://doi.org/10.1007/978-94-015-7644-4_1
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