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Appl. Phys. Lett. 92, 203304 (2008); doi:10.1063/1.2936085 (3 pages)

Observation of light-induced reorientational effects in periodic structures with planar nematic-liquid-crystal defects

Urszula A. Laudyn1,2, Andrey E. Miroshnichenko2, Wieslaw Krolikowski2, Deng Feng Chen2, Yuri S. Kivshar2, and Miroslaw A. Karpierz1

1Warsaw University of Technology, Faculty of Physics, Koszykowa 75, 00-662 Warsaw, Poland
2Nonlinear Physics Centre and Laser Physics Centre, Centre for Ultra-high Bandwidth Devices for Optical Systems (CUDOS), Australian National University, Canberra, ACT 0200, Australia

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(Received 25 March 2008; accepted 30 April 2008; published online 22 May 2008)

We report on the experimental studies of the light-induced reorientational effects in a one-dimensional periodic photonic structure with an embedded planar nematic-liquid-crystal defect. We demonstrate that in the presence of a periodic structure, the self-action of light in a liquid-crystal layer demonstrates sharp power-dependent characteristics for the intensity-dependent optical transmission. Robustness of the effect suggests its applications for all-optical tunable photonic devices.

© 2008 American Institute of Physics

KEYWORDS and PACS

PACS

  • 61.30.Gd

    Orientational order of liquid crystals; electric and magnetic field effects on order

  • 61.30.Jf

    Defects in liquid crystals

  • 42.70.Df

    Liquid crystals

PUBLICATION DATA

ISSN:

0003-6951 (print)  
1077-3118 (online)

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Figures (click on thumbnails to view enlargements)

FIG.1
(a) Schematic of the one-dimensional periodic structure with a liquid-crystal defect layer. (b) shows a sketch of molecular alignment in the liquid crystal; schematically shown molecular reorientation in the (x,y) plane; θ is the orientational angle, β is the angle between the direction of the electric field and the y coordinate. (c) Experimental (red) and theoretical (blue) transmission spectrum of the periodic structure with LC defect layer. (d) Zoom of the theoretical spectra near the pumping wavelength λ = 532 nm showing the existence of ordinary (β = 0°) and extraordinary (β = 90°) defect modes. In addition to this, we plot the variation of the transmission after reorientation, by assuming that Θ(z) = Θmax sin(πz/L).

FIG.1 Download High Resolution Image (.zip file) | Export Figure to PowerPoint

FIG.2
Experimental setup: M, mirrors, λ/2, waveplate, P, polarizer, L, lens, A, analyzer, S, screen, D, detector, and CCD camera. Linearly polarized light after polarizer and waveplate is focused on the front facet of the structure by means of lens with f = 100 mm. Polarizer and waveplate allow to control the polarization and input power.

FIG.2 Download High Resolution Image (.zip file) | Export Figure to PowerPoint

FIG.3
Transmission of the y-polarized light as a function of the input power. The insets show the light intensity distribution in the far field for the input power: (a) P 1.1 mW, (b) P 1.4 mW, (c) P 3.7 mW, and (d) P 4.2 mW.

FIG.3 Download High Resolution Image (.zip file) | Export Figure to PowerPoint

FIG.4
(a) Transmission for different angles of the initial linear light polarization (different values of β) vs the input power. The arrow indicates the shift of the transmission peak; (b) transmission spectra for periodic structure with 50 μm (dashed -black) and 12 μm (solid -red) thick liquid-crystal defect layer.

FIG.4 Download High Resolution Image (.zip file) | Export Figure to PowerPoint



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