Nematicon all-optical control in liquid crystal light valves

A. Alberucci; A. Piccardi; U. Bortolozzo; S. Residori; G. Assanto

doi:10.1364/OL.35.000390

Optics Letters
Vol. 35,
Issue 3,
pp. 390-392
(2010)
•https://doi.org/10.1364/OL.35.000390

Nematicon all-optical control in liquid crystal light valves

A. Alberucci, A. Piccardi, U. Bortolozzo, S. Residori, and G. Assanto

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A. Alberucci, A. Piccardi, U. Bortolozzo, S. Residori, and G. Assanto, "Nematicon all-optical control in liquid crystal light valves," Opt. Lett. 35, 390-392 (2010)

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Abstract

We discuss the interactions between self-guided light beams and light-induced perturbations in a liquid crystal light valve. The model and data are in perfect agreement.

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$D_{1 t}^{ψ ψ} = - \frac{ε_{t t}}{ε_{ξ ξ}} \cos^{2} δ^{(0)} - \sin^{2} δ^{(0)} - \frac{ε_{s t}}{ε_{ξ ξ}} \cos δ^{(0)} \sin δ^{(0)}$	$D_{2 t}^{ψ ψ} = (1 - \frac{ε_{t t}}{ε_{ξ ξ}}) \cos δ^{(0)} \sin δ^{(0)} - \frac{ε_{s t}}{ε_{ξ ξ}} \sin^{2} δ^{(0)}$
$D_{1 t}^{ψ ζ} = - (1 - \frac{ε_{t t}}{ε_{ξ ξ}}) \sin (2 δ^{(0)}) - \frac{ε_{s t}}{ε_{ξ ξ}} \cos (2 δ^{(0)})$	$D_{2 t}^{ψ ζ} = (1 - \frac{ε_{t t}}{ε_{ξ ξ}}) \cos (2 δ^{(0)}) - \frac{ε_{s t}}{ε_{ξ ξ}} \sin (2 δ^{(0)})$
$D_{1 t}^{ζ ζ} = - \frac{ε_{t t}}{ε_{ξ ξ}} \sin^{2} δ^{(0)} - \cos^{2} δ^{(0)} + \frac{ε_{s t}}{ε_{ξ ξ}} \cos δ^{(0)} \sin δ^{(0)}$	$D_{2 t}^{ζ ζ} = (\frac{ε_{t t}}{ε_{ξ ξ}} - 1) \sin δ^{(0)} \cos δ^{(0)} - \frac{ε_{s t}}{ε_{ξ ξ}} \cos^{2} δ^{(0)}$
$D_{1 s}^{ζ ζ} = \frac{ε_{s t}}{ε_{ξ ξ}} \sin^{2} δ^{(0)} - (\frac{ε_{s s}}{ε_{ξ ξ}} - 1) \cos δ^{(0)} \sin δ^{(0)}$	$D_{2 s}^{ζ ζ} = \frac{ε_{s s}}{ε_{ξ ξ}} \cos^{2} δ^{(0)} + \sin^{2} δ^{(0)} - \frac{ε_{s t}}{ε_{ξ ξ}} \cos δ^{(0)} \sin δ^{(0)}$

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