2015
DOI: 10.1103/physreve.92.052504
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Geometric phase ando-mode blueshift in a chiral anisotropic medium inside a Fabry-Pérot cavity

Abstract: Anomalous spectral shift of transmission peaks is observed in a Fabry-Pérot cavity filled with a chiral anisotropic medium. The effective refractive index value resides out of the interval between the ordinary and the extraordinary refractive indices. The spectral shift is explained by contribution of a geometric phase. The problem is solved analytically using the approximate Jones matrix method, numerically using the accurate Berreman method, and geometrically using the generalized Mauguin-Poincaré rolling co… Show more

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Cited by 12 publications
(17 citation statements)
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References 88 publications
(181 reference statements)
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“…This condition simulates the Mauguin’s regime in the LC layer for the transmitted light linearly polarized along the director or orthogonally to it on the input mirror. In contrast to the Mauguin’s regime, the propagation of waves in the TN-FPC is not waveguide, since the modes in the bulk of LC remain elliptically polarized 13,19 . The wavelength λ max  = 560 nm shown by the arrow in Fig.…”
Section: Resultsmentioning
confidence: 95%
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“…This condition simulates the Mauguin’s regime in the LC layer for the transmitted light linearly polarized along the director or orthogonally to it on the input mirror. In contrast to the Mauguin’s regime, the propagation of waves in the TN-FPC is not waveguide, since the modes in the bulk of LC remain elliptically polarized 13,19 . The wavelength λ max  = 560 nm shown by the arrow in Fig.…”
Section: Resultsmentioning
confidence: 95%
“…6b). Nevertheless, in view of the frequency closeness, the key parameters υ determining the direction of linear polarization of the cavity mode on the mirror 13,19 differ insignificantly even at the end points of the λ( U ) dependence in Fig. 6b, when the modes start diverging.…”
Section: Resultsmentioning
confidence: 95%
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“…Therefore, the phase variation by ϕ angle is not a dynamic phase, as it does not change the optical distance. Such a phase shift is called the geometric phase [39,40].…”
Section: Eigenmode Phase Matching Conditionmentioning
confidence: 99%
“…The extraordinary dielectric permittivity axis is collinear to the LC local director. As it was geometrically demonstrated in [4], the angle ξ between the linear polarization on the mirror and the LC director at the input mirror is determined by the Napier's rule:…”
Section: Figures 2a and 2bmentioning
confidence: 99%