Optical Property of Electro-Tunable Defect Mode in 1D Periodic
Structure with Light Crystal Defect Layer
Ryotaro Ozaki, Tatsunosuke Matsui, Masanori Ozaki, and Katsumi Yoshino
Graduate School of Engineering, Osaka University, Suita, 565-0871 Japan
SUMMARY
A liquid crystal defect layer is introduced into a
one-dimensional photonic crystal and its optical distance is
varied by an electric field so that the defect mode can be
controlled. An optical propagation simulation is carried out
for study of optical characteristics in a model in which
nematic liquid crystal is introduced as a liquid crystal defect
layer in a dielectric multilayer as a one-dimensional pho-
tonic crystal. We investigate whether the defect mode can
be controlled by varying the optical length by way of
change in orientation of the liquid crystal molecules. Based
on the simulation results, a device is fabricated with a
nematic defect layer introduced within a SiO
2
/TiO
2
lami-
nated periodic structure. The defect mode of the one-dimen-
sional photonic crystal is measured. It is confirmed that the
experimental results and the simulation results agree well.
Further, it is successful in shifting the defect mode wave-
length by applying a voltage. Hence, it is clear that the
defect mode can be modulated by changing the optical
length of the defect layer by means of control of the orien-
tation of the liquid crystal molecules by an applied voltage.
© 2004 Wiley Periodicals, Inc. Electron Comm Jpn Pt 2,
87(5): 2431, 2004; Published online in Wiley InterScience
(www.interscience.wiley.com). DOI 10.1002/ecjb.10167
Key words: photonic crystal; liquid crystal; defect
mode.
1. Introduction
Photonic crystals are materials with a completely new
concept that have a photonic bandgap in which the exist-
ence of light is forbidden when the medium has a periodic
structure on the order of the optical wavelength. If a defect
disturbing the periodicity is introduced into this photonic
crystal, localization of light is generated and a defect mode
appears within the photonic bandgap [1, 2]. This defect
mode can be applied to infinitesimal optical circuit devices
and lasers without thresholds. This technique is expected to
be important for the next-generation optoelectronics. Ex-
tensive research has been carried out worldwide both theo-
retically and experimentally [37].
On the other hand, liquid crystals are widely used for
display at present due to their characteristics of optical
anisotropy and dielectric anisotropy based on the orienta-
tion order. The present authors have proposed the use of
optical anisotropy caused by control of orientation of the
liquid crystal by temperature and electric field in the appli-
cation of photonic crystals [812]. Liquid crystals are in-
troduced into a three-dimensional photonic crystal using
self-assembly of colloidal particles such as opal and in-
verted opal. A tunable photonic crystal is realized in which
the photonic bandgap is shifted. It was demonstrated that
control of the photonic band is possible by electric fields
and temperature. However, in these three-dimensional sys-
tems, introduction of a defect is a problem. On the other
© 2004 Wiley Periodicals, Inc.
Electronics and Communications in Japan, Part 2, Vol. 87, No. 5, 2004
Translated from Denshi Joho Tsushin Gakkai Ronbunshi, Vol. J86-C, No. 5, May 2003, pp. 511517
Contract grant sponsor: Supported in part by a Scientific Research Grant
[Basic Research B(2) 14350165] from the Ministry of Education and
Science.
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