Computer calculations of refractive indices in orthoconic SmCA *. Is it possible to obtain “isotropic” antiferroelectric liquid crystal (IAFLC)?

2011 ◽  
Vol 19 (1) ◽  
Author(s):  
P. Perkowski ◽  
Z. Raszewski ◽  
W. Piecek ◽  
J. Kędzierski ◽  
J. Rutkowska ◽  
...  

AbstractOrthoconic antiferroelectric liquid crystals (OAFLC) are promising materials for applications. The saturated value of the tilt angle for such materials is 45°, while for “classical” antiferroelectric liquid crystals (AFLC) it reaches typically 30°. Homogeneously oriented slab of OAFLC, unwound by surface action of cell walls is apparently optically isotropic for the light beam at normal incidence. Such unwound structure of OAFLC one can call isotropic OAFLC (IOAFLC). Optical indicatrix of OAFLC is represented by an oblate sphere (ellipsoid of revolution) with its short axis perpendicular to cell walls. Here the question arises: “Is it possible to create isotropic AFLC (IAFLC)? An effective refractive index of IAFLC should have the same value for the light beam propagating at each direction, hence the optical indicatrix should be a sphere. In the way of theoretical considerations we found that IAFLC can exist for twisted structure of AFLC characterized by the tilt angle as high as 54.3°. Unfortunately, such a big tilt angle is still not achievable in practice. Calculations show that AFLC can be optically isotropic when the helix is not suppressed by cell walls action.

2007 ◽  
Vol 15 (1) ◽  
Author(s):  
A. Spadło ◽  
N. Bennis ◽  
R. Dąbrowski ◽  
X. Quintana ◽  
J. Otón ◽  
...  

AbstractOrthoconic antiferroelectric liquid crystals (AFLCs) having 45° tilt angle have been proposed to overcome the problem of reduced contrast usually exhibited by regular antiferroelectric displays. However, the pitch of the helix induced by chirality is customarily short in existing orthoconic materials, making it difficult to achieve surface stabilized configurations when the material’s pitch is smaller than the cell thickness.In this work, the influence of different manufacturing procedures on the electrooptical behaviour of orthoconic AFLCs is studied. Using the same orthoconic AFLC mixture, aligning surfaces and manufacturing protocol, we have observed two dissimilar responses, true orthoconic behaviour, and orthoconic V-shape response. The electrooptical response depends ultimately on the rubbing strategy adopted in either case.


1997 ◽  
Vol 7 (12) ◽  
pp. 1817-1828 ◽  
Author(s):  
P. Gisse ◽  
M. Sidir ◽  
V. L. Lorman ◽  
R. Farhi ◽  
J. Pavel ◽  
...  

1996 ◽  
Vol 25 (8) ◽  
pp. 583-584 ◽  
Author(s):  
Makoto Negishi ◽  
Kiyoshi Kanie ◽  
Tomiki Ikeda ◽  
Tamejiro Hiyama

2019 ◽  
Author(s):  
Richard Mandle ◽  
John W. Goodby

We compare the order parameters, orientational distribution functions (ODF) and heliconical tilt angles of the TB phase exhibited by a liquid-crystalline dimer (CB7CB) to a tetramer (O47) and hexamer (O67) by SAXS/WAXS. Following the N-TB phase transition we find that all order parameters decrease, and while 〈P2 〉 remains positive 〈P4 〉 becomes negative. For all three materials the order parameter 〈P6 〉 is near zero in both phases. The ODF is sugarloaf-like in the nematic phase and volcano-like in the TB phase, allowing us to estimate the heliconical tilt angle of each material and its thermal evolution. The heliconical tilt angle appears to be largely independent of the material studied despite the differing number of mesogenic units.


2002 ◽  
Vol 33 (1) ◽  
pp. 770 ◽  
Author(s):  
Roman Dabrowski ◽  
Krzysztof Czupryński ◽  
Witold Drzewinski ◽  
Sebastian Gauza ◽  
Sven T. Lagerwall ◽  
...  

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