THESIS
2014
iv leaves, v-xvi, 144 pages : illustrations ; 30 cm
Abstract
The ferroelectric liquid crystal (FLC) which has the advantage of a fast response under an
electrical field has become one of the most promising candidates of the next generation
liquid crystal display (LCD) as well as photonic devices. In the display area, sub-millisecond
switching is needed to enable field sequential color (FSC) display technology,
which improves resolution and efficiency by three times when using sequentially coming
RGB colors instead of color filters. The FLC allows electrical control of the response time
in the range from several microseconds to several seconds. FLC devices also have a great
potential in the sensing and detection area since a microsecond response is in high demand
for real time sensors. Gratings, optical switches and phase modulators can al...[
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The ferroelectric liquid crystal (FLC) which has the advantage of a fast response under an
electrical field has become one of the most promising candidates of the next generation
liquid crystal display (LCD) as well as photonic devices. In the display area, sub-millisecond
switching is needed to enable field sequential color (FSC) display technology,
which improves resolution and efficiency by three times when using sequentially coming
RGB colors instead of color filters. The FLC allows electrical control of the response time
in the range from several microseconds to several seconds. FLC devices also have a great
potential in the sensing and detection area since a microsecond response is in high demand
for real time sensors. Gratings, optical switches and phase modulators can also be fabricated
with FLC, and can be applied in the optical communication area.
Among various electrooptical modes of FLC, the surface stabilized ferroelectric liquid
crystal (SSFLC) shows intrinsic bi-stability and response time of order microsecond. But a
continuously tunable threshold free phase shift of light, which is important for photonic and
display application is rarely possible with SSFLC. On the other hand, deformed helix
ferroelectric (DHF) mode can provide a continuously tunable and hysteresis-free phase
modulation. The characteristics of DHF cells in a transmissive and reflective regime are
investigated. Several application cases of DHF mode are discussed.
Recently, we have proposed a novel electrooptical mode, the so called electrically
suppressed helix (ESH) mode, which offers good alignment quality, high contrast ratio and
low driving voltage. The self-diffractive scattering of ESH cells is extremely low. Owing to
the good alignment quality, we can apply the patterned alignment method to generate the
periodic distribution of the refractive index and thus the switchable grating. The FSC display based on ESH mode exhibits a high contrast ratio and fast response, as well as a
wide viewing angle.
The aligning method is a critical issue for FLC devices. The photoaligning technique is in
high demand compared with the traditional rubbing method, since photoaligning is a non-contact
process which avoids static charges, particles, and contacting damages. Furthermore,
the photoaligning technique can realize controllable anchoring energy by exposure dose. So
far, among the photosensitive materials, azo-dye material SD1 provides best alignment
quality for both ESH and DHF cells. A method to obtain optimal alignment quality by
balancing the elastic energy of helix and the anchoring energy of the alignment layer is
proposed. The photo-stability of azo-dye SD1 is improved using a composite layer with
SD1 and photosensitive polymer.
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