Electro-tuning of the photonic band gap in SOI-based structures infiltrated with liquid crystal

One dimensional periodic and non-periodic silicon photonic structures have been designed and fabricated on silicon-on-insulator substrate for the investigation of the electro-tuning effect in composite system Photonic Crystal - Liquid Crystal. The reflection spectra registered for non-periodic structures demonstrate the phase polarisation shift for bands of high reflection, while for the periodic structure the shift of the photonic band gap edge was observed. Under an applied electric field in the range from 2V to 10V, the shift of the polarised reflection spectra, caused by reorientation of the LC director from planar to homeotropic alignment, has been obtained. A significant change in the refractive index close to Δn=0.2, which is a characteristic feature for LC E7, has been achieved due to LC reorientation in all structures just after LC infiltration. It was found that after switching-off the applied electric field the initial planar orientation of LC molecules is not restored. This effect is related to weak anchoring of LC molecules to the silicon side-walls which results in the transition of LC to the pseudo-isotropic alignment after the applied voltage is off. A relatively smaller (with Δn=0.07), but highly reproducible electro-tuning effect was revealed during the LC reorientation from pseudo-isotropic to homeotropic alignment. The shift of the edge of PBG by Δλ=0.16 or by Δλ/λ=1.6% in relative shift units was observed in this case. The response time estimated under applied square shaped ac pulses of various frequencies was found to be around 30 ms.

[1]  E. Yablonovitch,et al.  Inhibited spontaneous emission in solid-state physics and electronics. , 1987, Physical review letters.

[2]  L. Blinov Electro-optical and Magneto-optical Properties of Liquid Crystals , 1983 .

[3]  Electrotunable in-plane one-dimensional photonic structure based on silicon and liquid crystal , 2007 .

[4]  Masanori Ozaki,et al.  Electrically color-tunable defect mode lasing in one-dimensional photonic-band-gap system containing liquid crystal , 2003 .

[5]  E. H. Linfoot Principles of Optics , 1961 .

[6]  Iam-Choon Khoo,et al.  The Infrared Optical Nonlinearities of Nematic Liquid Crystals and Novel Two-wave Mixing Processes , 1990 .

[7]  R. Baughman,et al.  Electro-optic behavior of liquid-crystal-filled silica opal photonic crystals: effect of liquid-crystal alignment. , 2001, Physical review letters.

[8]  Philippe M. Fauchet,et al.  Electrically tunable porous silicon active mirrors , 2003 .

[9]  Jong-Hyun Lee,et al.  A micromachined in-plane tunable optical filter using the thermo-optic effect of crystalline silicon , 2003 .

[10]  T. Perova,et al.  1D photonic crystal fabricated by wet etching of silicon , 2005 .

[11]  Shin-Tson Wu,et al.  Electrically tunable liquid-crystal photonic crystal fiber , 2004 .

[12]  T. Perova,et al.  Electro-tunable one-dimensional photonic crystal structures based on grooved silicon infiltrated with liquid crystal , 2006 .

[13]  N. Daldosso,et al.  Silicon-based near-infrared tunable filters filled with positive or negative dielectric anisotropic liquid crystals , 2004 .

[14]  R. Azzam,et al.  Ellipsometry and polarized light , 1977 .

[15]  Anders Bjarklev,et al.  Continuously tunable devices based on electrical control of dual-frequency liquid crystal filled photonic bandgap fibers. , 2005, Optics express.

[16]  Osamu Sato,et al.  Effects of external electric field upon the photonic band structure in synthetic opal infiltrated with liquid crystal , 2001 .

[17]  John,et al.  Strong localization of photons in certain disordered dielectric superlattices. , 1987, Physical review letters.

[18]  E. Graugnard,et al.  Electric-field tuning of the Bragg peak in large-pore Ti O 2 inverse shell opals , 2005 .