Liquid Crystals: Difference between revisions

From PhyWiki
Jump to navigation Jump to search
Line 13: Line 13:
== Isotropic, nematic and cholesteric phases[4] ==
== Isotropic, nematic and cholesteric phases[4] ==


=== Structure Factor ===
=== Density Correlation and Structure Factor ===


A lot of information about the bulk structure of LCDs can be obtained via scattering of X-rays. let <math>|\boldsymbol{k}\rangle</math> and <math>|\boldsymbol{k}^{'}\rangle</math> be the incident and final plane wave state of the scattered particle with respective momenta <math>\hbar\boldsymbol{k}</math> and <math>\hbar\boldsymbol{k}^{'}</math> If the scattered particle interacts weakly with the scaterring medium via a sufficiently short-ranged interaction <math>U</math>, then by Fermi's Golden rule, the transition rate between <math>|\boldsymbol{k}\rangle</math> and <math>|\boldsymbol{k}^{'}\rangle</math> is proportional to the square of the matrix element,
A lot of information about the bulk structure of LCDs can be obtained via scattering of X-rays. let <math>|\boldsymbol{k}\rangle</math> and <math>|\boldsymbol{k}^{'}\rangle</math> be the incident and final plane wave state of the scattered particle with respective momenta <math>\hbar\boldsymbol{k}</math> and <math>\hbar\boldsymbol{k}^{'}</math> If the scattered particle interacts weakly with the scaterring medium via a sufficiently short-ranged interaction <math>U</math>, then by Fermi's Golden rule, the transition rate between <math>|\boldsymbol{k}\rangle</math> and <math>|\boldsymbol{k}^{'}\rangle</math> is proportional to the square of the matrix element,
Line 26: Line 26:
where <math>\boldsymbol{x^{'}}</math> is the position of the atom labeled <math>\alpha</math>. the matrix element, therefore, is
where <math>\boldsymbol{x^{'}}</math> is the position of the atom labeled <math>\alpha</math>. the matrix element, therefore, is


<math>\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum^{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.\boldsymbol{x}}U_{\alpha}(\boldsymbol{x}-\boldsymbol{x_{\alpha}})e^{i\boldsymbol{k^{'}}.\boldsymbol{x}}</math>
<math>\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum_{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.\boldsymbol{x}}U_{\alpha}(\boldsymbol{x}-\boldsymbol{x_{\alpha}})e^{i\boldsymbol{k^{'}}.\boldsymbol{x}}</math>


To seperate the potential interaction and the interatomic correlation factors, we shift our centers to each <math>x_{\alpha}</math>. Let <math>\boldsymbol{R}_{\alpha} = \boldsymbol{x}-\boldsymbol{x_{\alpha}}</math>.
To seperate the potential interaction and the interatomic correlation factors, we shift our centers to each <math>x_{\alpha}</math>. Let <math>\boldsymbol{R}_{\alpha} = \boldsymbol{x}-\boldsymbol{x_{\alpha}}</math>.


<math>\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum^{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})}U_{\alpha}(\boldsymbol{R}_{\alpha})e^{i\boldsymbol{k^{'}}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})} </math>
<math>\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum_{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})}U_{\alpha}(\boldsymbol{R}_{\alpha})e^{i\boldsymbol{k^{'}}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})} </math>
<math>= \sum^{\alpha}[\int d^{d}x e^{-i\boldsymbol{q}.\boldsymbol{R}_{\alpha}}U_{\alpha}(\boldsymbol{R}_{\alpha})]e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}</math>
<math>= \sum_{\alpha}[\int d^{d}x e^{-i\boldsymbol{q}.\boldsymbol{R}_{\alpha}}U_{\alpha}(\boldsymbol{R}_{\alpha})]e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}</math>
<math>=\sum^{\alpha}U_{\alpha}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}</math>
<math>=\sum_{\alpha}U_{\alpha}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}</math>
Here the scattering wave vector is <math>\boldsymbol{q} = \boldsymbol{k} - \boldsymbol{k}^{'}</math> and <math>U_{\alpha}(\boldsymbol{q})</math> is the atomic form factor, which is nothing but the Fourier transform of the atomic potential. The differential cross-section is proportional to the matrix element squared:
Here the scattering wave vector is <math>\boldsymbol{q} = \boldsymbol{k} - \boldsymbol{k}^{'}</math> and <math>U_{\alpha}(\boldsymbol{q})</math> is the atomic form factor, which is nothing but the Fourier transform of the atomic potential. The differential cross-section is proportional to the matrix element squared:
<math>|\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle|^{2} = \sum^{\alpha,\alpha^{'}}U_{\alpha}(\boldsymbol{q})U_{\alpha^{'}}^{*}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}e^{i\boldsymbol{q}.\boldsymbol{x}_{\alpha^{'}}}</math>
<math>|\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle|^{2} = \sum_{\alpha,\alpha^{'}}U_{\alpha}(\boldsymbol{q})U_{\alpha^{'}}^{*}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}e^{i\boldsymbol{q}.\boldsymbol{x}_{\alpha^{'}}}</math>
 
If the positions of atoms are rigidly fixed,then this expression gives the exact answer. However, in real materials, the particles move around,probing large regions of phase space consistent with statistical mechanics, and we need an ensemble average of the ideal cross-section. Under ergodic hypothesis and assuming the particles are identical,
<math>\frac{\mathrm{d}^{2}\sigma }{\mathrm{d} \Omega}\sim |U_{\alpha}(\boldsymbol{q})|^{2}\boldsymbol{I}(\boldsymbol{q})</math>
where the function
 
<math>\boldsymbol{I}(\boldsymbol{q}) = \left \langle\sum_{\alpha,\alpha^{'}}e^{-i\boldsymbol{q}.(\boldsymbol{x}_{\alpha}-\boldsymbol{x_{\alpha^{'}}})}\right \rangle</math>
is called the structure function. As intensive version of the structure function is called the structure factor.
 
<math>S(\boldsymbol{q}) = \frac{\boldsymbol{I}(\boldsymbol{q})}{N} </math> or <math>S(\boldsymbol{q}) = \frac{\boldsymbol{I}(\boldsymbol{q})}{V}</math>

Revision as of 00:31, 24 November 2010

Introduction

Homogeneous, isotropic liquids have an average structure that is invariant under arbitrary rotations and translations.It has no long range order, and has the highest possible symmetry with maximum possible entropy.The crystalline state has long range translational and rotational order, with the lowest possible symmetry consistent with a regular filling of space. Between these two, there are systems which exhibit short range correlations in some directions and long range in others, and have symmetries intermediate between between those of liquids and crystals.

Among the materials that show intermediate order, the most widely studied are liquid crystals.Liquid crystals are usually made of strongly anisotropic organic molecules, either elongated (calamitic, rod-like molecules) or disk-like (discotic molecules). As a rule, the inner part of mesogenic molecules is rigid (e.g. phenyl groups) and the outer part flexible (aliphatic chains). This double character explains altogether the existence of steric interactions (between rod-like or disk-like cores) yielding orientational order and the fluidity of the mesomorphic phases. Typical examples are cyanobiphenyls and MBBA. These produce thermotropic mesophases,i.e. phases with a single component, whose phase transitions can be induced by a change in temperature.The other broad LC class is constituted by the lyotropic mesophases: they occur when anisotropic amphiphilic molecules (soaps, phospholipids, various types of surfactant molecules and biomolecules) are added to a solvent. Because amphiphiles have two distinct parts, a polar head and a non-polar tail,the building units of lyotropic phases are usually aggregates of many molecules(micelles) rather than single molecules. This microphase separation dominating the lyotropic behavior is partly present also in thermotropic LC, as for example in the smectic phases, where polar and non polar portions of the molecules form distinct alternatinig planes in the system.A typical example of lyotropics is a water solution of SDS, sodium dodecyl sulphate. For concentrations above the critical micellar concentration, cmc, these molecules form aggregates of different shapes, spherical or cylindrical micelles,bilayers, inverse cylinders, and inverse micelles.[1,2.3]


Classification of LC phases

LCs show many possible structures, which can belong to the same compound (polymorphism). There are four basic types of liquid crystalline phases, classified accordingly to the dimensionality of the translational correlations of building units: nematic (no translational correlations), smectic (1D correlation),columnar (2D) and various 3D-correlated structures, such as cubic phases.


Isotropic, nematic and cholesteric phases[4]

Density Correlation and Structure Factor

A lot of information about the bulk structure of LCDs can be obtained via scattering of X-rays. let Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\boldsymbol{k}\rangle} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\boldsymbol{k}^{'}\rangle} be the incident and final plane wave state of the scattered particle with respective momenta Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \hbar\boldsymbol{k}} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \hbar\boldsymbol{k}^{'}} If the scattered particle interacts weakly with the scaterring medium via a sufficiently short-ranged interaction Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle U} , then by Fermi's Golden rule, the transition rate between Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\boldsymbol{k}\rangle} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\boldsymbol{k}^{'}\rangle} is proportional to the square of the matrix element,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle M_{\boldsymbol{k},\boldsymbol{k^{'}}} = \langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \int d^{d}x e^{-i\boldsymbol{k}.\boldsymbol{x}}U(\boldsymbol{x})e^{i\boldsymbol{k^{'}}.\boldsymbol{x}} }

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle U(\boldsymbol{x})} is the scattering potential in the coordinate representation of the scattered particle, and our plane wave states are unnormalized.

In multiparticle systems, the scattering potential is the sum of terms from individual atoms in the material:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle U(\boldsymbol{x}) = \sum_{\alpha} U_{\alpha}(\boldsymbol{x}-\boldsymbol{x^{'}})} where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \boldsymbol{x^{'}}} is the position of the atom labeled Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha} . the matrix element, therefore, is

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum_{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.\boldsymbol{x}}U_{\alpha}(\boldsymbol{x}-\boldsymbol{x_{\alpha}})e^{i\boldsymbol{k^{'}}.\boldsymbol{x}}}

To seperate the potential interaction and the interatomic correlation factors, we shift our centers to each Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x_{\alpha}} . Let Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \boldsymbol{R}_{\alpha} = \boldsymbol{x}-\boldsymbol{x_{\alpha}}} .

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle = \sum_{\alpha}\int d^{d}x e^{-i\boldsymbol{k}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})}U_{\alpha}(\boldsymbol{R}_{\alpha})e^{i\boldsymbol{k^{'}}.(\boldsymbol{x}_{\alpha}+\boldsymbol{R}_{\alpha})} } Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle = \sum_{\alpha}[\int d^{d}x e^{-i\boldsymbol{q}.\boldsymbol{R}_{\alpha}}U_{\alpha}(\boldsymbol{R}_{\alpha})]e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}} Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle =\sum_{\alpha}U_{\alpha}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}} Here the scattering wave vector is Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \boldsymbol{q} = \boldsymbol{k} - \boldsymbol{k}^{'}} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle U_{\alpha}(\boldsymbol{q})} is the atomic form factor, which is nothing but the Fourier transform of the atomic potential. The differential cross-section is proportional to the matrix element squared: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\langle\boldsymbol{k}|U|\boldsymbol{k^{'}}\rangle|^{2} = \sum_{\alpha,\alpha^{'}}U_{\alpha}(\boldsymbol{q})U_{\alpha^{'}}^{*}(\boldsymbol{q})e^{-i\boldsymbol{q}.\boldsymbol{x}_{\alpha}}e^{i\boldsymbol{q}.\boldsymbol{x}_{\alpha^{'}}}}

If the positions of atoms are rigidly fixed,then this expression gives the exact answer. However, in real materials, the particles move around,probing large regions of phase space consistent with statistical mechanics, and we need an ensemble average of the ideal cross-section. Under ergodic hypothesis and assuming the particles are identical,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{\mathrm{d}^{2}\sigma }{\mathrm{d} \Omega}\sim |U_{\alpha}(\boldsymbol{q})|^{2}\boldsymbol{I}(\boldsymbol{q})} where the function

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \boldsymbol{I}(\boldsymbol{q}) = \left \langle\sum_{\alpha,\alpha^{'}}e^{-i\boldsymbol{q}.(\boldsymbol{x}_{\alpha}-\boldsymbol{x_{\alpha^{'}}})}\right \rangle} is called the structure function. As intensive version of the structure function is called the structure factor.

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle S(\boldsymbol{q}) = \frac{\boldsymbol{I}(\boldsymbol{q})}{N} } or Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle S(\boldsymbol{q}) = \frac{\boldsymbol{I}(\boldsymbol{q})}{V}}

Retrieved from "http://wiki.physics.fsu.edu/index.php?title=Liquid_Crystals&oldid=8738"