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Revision 2780 by tim, Mon Apr 3 18:07:54 2006 UTC vs.
Revision 2781 by tim, Wed May 31 04:29:44 2006 UTC

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1   \chapter{\label{chapt:liquidcrystal}LIQUID CRYSTAL}
2  
3   \section{\label{liquidCrystalSection:introduction}Introduction}
4 + % liquid crystal
5  
6 + Long range orientational order is one of the most fundamental
7 + properties of liquid crystal mesophases. This orientational
8 + anisotropy of the macroscopic phases originates in the shape
9 + anisotropy of the constituent molecules. Among these anisotropy
10 + mesogens, rod-like (calamitic) and disk-like molecules have been
11 + exploited in great detail in the last two decades. Typically, these
12 + mesogens consist of a rigid aromatic core and one or more attached
13 + aliphatic chains. For short chain molecules, only nematic phases, in
14 + which positional order is limited or absent, can be observed,
15 + because the entropy of mixing different parts of the mesogens is
16 + paramount to the dispersion interaction. In contrast, formation of
17 + the one dimension lamellar sematic phase in rod-like molecules with
18 + sufficiently long aliphatic chains has been reported, as well as the
19 + segregation phenomena in disk-like molecules.
20 +
21 + % banana shaped
22 + Recently, the banana-shaped or bent-core liquid crystal have became
23 + one of the most active research areas in mesogenic materials and
24 + supramolecular chemistry. Unlike rods and disks, the polarity and
25 + biaxiality of the banana-shaped molecules allow the molecules
26 + organize into a variety of novel liquid crystalline phases which
27 + show interesting material properties. Of particular interest is the
28 + spontaneous formation of macroscopic chiral layers from achiral
29 + banana-shaped molecules, where polar molecule orientational ordering
30 + is shown within the layer plane as well as the tilted arrangement of
31 + the molecules relative to the polar axis. As a consequence of
32 + supramolecular chirality, the spontaneous polarization arises in
33 + ferroelectric (FE) and antiferroelectic (AF) switching of smectic
34 + liquid crystal phases, demonstrating some promising applications in
35 + second-order nonlinear optical devices.
36 +
37 + The most widely investigated mesophase formed by banana-shaped
38 + moleculed is the $\text{B}_2$ phase, which is also known as
39 + $\text{SmCP}$.
40 +
41 + %Previous Theoretical Studies
42 +
43   \section{\label{liquidCrystalSection:model}Model}
44  
45   \section{\label{liquidCrystalSection:methods}Methods}

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