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		<summary type="html">&lt;p&gt;142.205.241.253: /* Simple margin */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A &#039;&#039;&#039;biaxial nematic&#039;&#039;&#039; is a spatially homogeneous [[liquid crystal]] with three distinct optical axes. This is to be contrasted to a simple [[nematic]], which has a single preferred axis, around which the system is rotationally symmetric. The [[symmetry group]] of a biaxial nematic is &amp;lt;math&amp;gt;D_{2h}&amp;lt;/math&amp;gt; i.e. that of a rectangular right parallelepiped, having 3 orthogonal &amp;lt;math&amp;gt;C_2&amp;lt;/math&amp;gt; axes and three orthogonal mirror planes. In a frame co-aligned with optical axes the second rank [[order parameter]] [[tensor]] of a biaxial nematic has the form &lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
Q=&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
-\frac{1}{2}S+T &amp;amp; 0 &amp;amp;0 \\&lt;br /&gt;
0 &amp;amp;-\frac{1}{2}S-T &amp;amp; 0 \\&lt;br /&gt;
0 &amp;amp; 0&amp;amp; S\\&lt;br /&gt;
\end{pmatrix} &lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is the standard nematic scalar order parameter&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; a measure of the biaxiality. &lt;br /&gt;
&lt;br /&gt;
The first report of a thermotropic biaxial nematic appeared in 2004&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Madsen |first1=L. A.&lt;br /&gt;
 |last2=Dingemans |first2=T. J.&lt;br /&gt;
 |last3=Nakata |first3=M.&lt;br /&gt;
 |last4=Samulski |first4=E. T.&lt;br /&gt;
 |year=2004&lt;br /&gt;
 |title=Thermotropic Biaxial Nematic Liquid Crystals&lt;br /&gt;
 |journal=[[Physical Review Letters]]&lt;br /&gt;
 |volume=92 |pages=145505&lt;br /&gt;
 |doi=10.1103/PhysRevLett.92.145505 |pmid=15089552 |bibcode=2004PhRvL..92n5505M&lt;br /&gt;
 |issue=14&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Prasad |first1=V.&lt;br /&gt;
 |last2=Kang |first2=S.-Woong&lt;br /&gt;
 |last3=Suresh |first3=K. A.&lt;br /&gt;
 |last4=Joshi |first4=Leela&lt;br /&gt;
 |last5=Wang |first5=Qingbing&lt;br /&gt;
 |last6=Kumar |first6=Satyendra&lt;br /&gt;
 |year=2005&lt;br /&gt;
 |title=Thermotropic Uniaxial and Biaxial Nematic and Smectic Phases in Bent-Core Mesogens&lt;br /&gt;
 |journal=[[Journal of the American Chemical Society]]&lt;br /&gt;
 |volume=127 |pages=17224&lt;br /&gt;
 |doi=10.1021/ja052769n&lt;br /&gt;
 |issue=49&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;  based on a [[boomerang]] shaped [[oxadiazole]] &#039;&#039;&#039;bent-core mesogen&#039;&#039;&#039;. The biaxial nematic phase for this particular compound only occurs at temperatures around 200 °C and is preceded by as yet unidentified [[smectic]] phases.&lt;br /&gt;
&lt;br /&gt;
[[Image:Biaxialnematic.gif|center|Biaxial nematic boomerang liquid crystal]]&lt;br /&gt;
&lt;br /&gt;
It is also found that this material can segregate into [[Chirality (chemistry)|chiral]] domains of opposite handedness.&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Görtz |first1=V.&lt;br /&gt;
 |last2=Goodby |first2=J. W.&lt;br /&gt;
 |year=2005&lt;br /&gt;
 |title=Enantioselective segregation in achiral nematic liquid crystals&lt;br /&gt;
 |journal=[[Chemical Communications]]&lt;br /&gt;
 |pages=3262&lt;br /&gt;
 |doi=10.1039/B503846D&lt;br /&gt;
 |issue=26&lt;br /&gt;
}}&amp;lt;/ref&amp;gt; For this to happen the boomerang shaped molecules adopt a helical superstructure.&lt;br /&gt;
&lt;br /&gt;
In one azo bent-core mesogen a thermal transition is found from a uniaxial N&amp;lt;sub&amp;gt;u&amp;lt;/sub&amp;gt; to a  biaxial nematic N&amp;lt;sub&amp;gt;b&amp;lt;/sub&amp;gt; mesophase,&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Prasad |first1=V.&lt;br /&gt;
 |last2=Kang |first2=S.-W.&lt;br /&gt;
 |last3=Suresh |first3=K. A.&lt;br /&gt;
 |last4=Joshi |first4=L.&lt;br /&gt;
 |last5=Wang |first5=Q.&lt;br /&gt;
 |last6=Kumar |first6=S.&lt;br /&gt;
 |year=2005&lt;br /&gt;
 |title=Thermotropic Uniaxial and Biaxial Nematic and Smectic Phases in Bent-Core Mesogens&lt;br /&gt;
 |journal=[[Journal of the American Chemical Society]]&lt;br /&gt;
 |volume=127 |pages=17224&lt;br /&gt;
 |doi=10.1021/ja052769n&lt;br /&gt;
 |issue=49 &lt;br /&gt;
}}&amp;lt;/ref&amp;gt; as predicted by theory and simulation.&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Bates |first1=M.&lt;br /&gt;
 |last2=Luckhurst |first2=G.&lt;br /&gt;
 |year=2005&lt;br /&gt;
 |title=Biaxial nematic phases and V-shaped molecules: A Monte Carlo simulation study&lt;br /&gt;
 |journal=[[Physical Review E]]&lt;br /&gt;
 |volume=72 |pages=051702&lt;br /&gt;
 |doi=10.1103/PhysRevE.72.051702&lt;br /&gt;
|bibcode = 2005PhRvE..72e1702B&lt;br /&gt;
 |issue=5 }}&amp;lt;/ref&amp;gt; This transition is observed on heating from the N&amp;lt;sub&amp;gt;u&amp;lt;/sub&amp;gt; phase with [[Polarizing optical microscopy]] as a change in [[Schlieren texture]] and increased light transmittance and from [[x-ray diffraction]] as the splitting of the nematic reflection. The transition is a [[Phase transition|second order transition]] with low energy content and therefore not observed in [[differential scanning calorimetry]]. The positional order parameter for the uniaxial nematic phase is 0.75 to 1.5 times the mesogen length and for the biaxial nematic phase 2 to 3.3 times the mesogen length.&lt;br /&gt;
&lt;br /&gt;
[[Image:Biaxialnematic2005.png|center|600px|Azo bent-core mesogen thermal transitions in °C: K 82.8 Sy 93.4 Sx 104.3 Sc 118.5 Nb 149 Nu 176.5 I]]&lt;br /&gt;
&lt;br /&gt;
Another strategy towards biaxial nematics is the use of mixtures of classical rodlike mesogens and disklike [[discotic]] mesogens.  The biaxial nematic phase is expected to be located below the minimum in the rod-disk phase diagram. In one study&amp;lt;ref&amp;gt;&lt;br /&gt;
{{cite journal&lt;br /&gt;
 |last1=Apreutesei |first1=D.&lt;br /&gt;
 |last2=Mehl |first2=G. H.&lt;br /&gt;
 |year=2006&lt;br /&gt;
 |title=Completely miscible disc and rod shaped molecules in the nematic phase&lt;br /&gt;
 |journal=[[Chemical Communications]]&lt;br /&gt;
 |pages=609&lt;br /&gt;
 |doi=10.1039/b512120e&lt;br /&gt;
 |issue=6&lt;br /&gt;
}}&amp;lt;/ref&amp;gt; a miscible system of rods and disks is actually found although the biaxial nematic phase remains elusive.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Chromonic]]&lt;br /&gt;
* [[Liquid crystal]]&lt;br /&gt;
* [[Liquid crystal display]]&lt;br /&gt;
* [[Liquid crystal polymer]]&lt;br /&gt;
* [[Lyotropic liquid crystal]]&lt;br /&gt;
* [[Plastic crystallinity]]&lt;br /&gt;
* [[Smart glass]]&lt;br /&gt;
* [[Thermochromics]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Phases of matter]]&lt;br /&gt;
[[Category:Crystallography]]&lt;br /&gt;
[[Category:Liquid crystals]]&lt;/div&gt;</summary>
		<author><name>142.205.241.253</name></author>
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