Biaxial nematic

A biaxial nematic 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 $D\_\{2h\}$ i.e. that of a rectangular right parallelepiped, having 3 orthogonal $C\_2$ 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 :

where

$S$ is the standard nematic scalar order parameter

$T$ a measure of the biaxiality.

The first report of a biaxial nematic appeared in 2004 Ref|Madsen Ref|Acharya based on a boomerang shaped oxadiazole bent-core mesogen. The biaxial nematic phase for this particular compound only occurs at temperatures around 200 °C and is preceded by as yet unidentified smectic phases.

It is also found that this material can segregate into chiral domains of opposite handedness Ref|Görtz For this to happen the boomerang shaped molecules adopt a helical superstructure.

In one azo bent-core mesogen a thermal transition is found from a uniaxial N_u to a biaxial nematic N_b mesophase Ref|Prasad, as predicted by theory and simulation Ref|simulation. This transition is observed on heating from the N_u 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 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.

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 Ref|Apreutesei a miscible system of rods and disks is actually found although the biaxial nematic phase remains elusive.

ee also

References

# "The elusive thermotropic biaxial nematic phase in rigid bent-core molecules", B. R. Acharya, A. Primak, T. J. Dingemans, E. T. Samulski, and S. Kumar, Pramana, 61, 231 (2003); "Biaxial Nematic Phase in Bent-Core Thermotropic Mesogens" Bharat R. Acharya, Andrew Primak, and Satyendra Kumar Phys. Rev. Lett. 92, 145506 (2004) [http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=PRLTAO000092000014145506000001&idtype=cvips&gifs=yes Abstract]
# "Thermotropic Biaxial Nematic Liquid Crystals" L. A. Madsen, T. J. Dingemans, M. Nakata, and E. T. Samulski Phys. Rev. Lett. 92, 145505 (2004) [http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=PRLTAO000092000014145505000001&idtype=cvips&gifs=yes Abstract]
# "Enantioselective segregation in achiral nematic liquid crystals" Verena Görtz and John W. Goodby Chemical Communications, 2005, (26), 3262 - 3264 [http://www.rsc.org/publishing/journals/CC/article.asp?doi=b503846d Abstract]
#Note|abd "Thermotropic Uniaxial and Biaxial Nematic and Smectic Phases in Bent-Core Mesogens" Veena Prasad, Shin-Woong Kang, K. A. Suresh, Leela Joshi, Qingbing Wang, and Satyendra Kumar J. Am. Chem. Soc., 127 (49), 17224 -17227, 2005
#Note|simulation "Biaxial nematic phases and V-shaped molecules: A Monte Carlo simulation study" Martin A. Bates and Geoffrey R. Luckhurst, Phys. Rev. E 72 051702 (2005). [http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=PLEEE8000072000005051702000001&idtype=cvips&gifs=yes Abstract] .
#Note|Apreutesei "Completely miscible disc and rod shaped molecules in the nematic phase" Daniela Apreutesei and Georg H. Mehl Chemical Communications, 2006, 609 - 611 [http://dx.doi.org/10.1039/b512120e graphical abstract]