Biaxial Nematics: Order Parameters and Distribution Functions

2015 ◽  
pp. 25-53 ◽  
Author(s):  
Geoffrey R. Luckhurst
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.


2005 ◽  
Vol 59 (3) ◽  
pp. 322-328 ◽  
Author(s):  
V. Rodriguez ◽  
F. Lagugné-Labarthet ◽  
C. Sourisseau

The most probable orientational distribution functions of rod-like polar molecules contained in a noncentrosymmetric uniaxial system are established using the first-rank and third-rank Legendre polynomials, 〈 P1(cos θ)〉 and 〈 P3(cos θ)〉 order parameters, and the maximum entropy method. Emphasis is put on the different domains of existence in the (〈 P1〉, 〈 P3〉) plane for the various shapes of the distributions: it is thus shown that, for any positive 〈 P1(cos θ)〉 value and for decreasing 〈 P3(cos θ)〉 values, the distribution function may exhibit either a distorted oblate form with an intense maximum at 0°, or a three-leaved rose curve with maxima at 60°, 180°, and 300°, and finally another markedly oblate shape with a strong maximum at 180°. As an illustrative example, we have considered the azobenzene molecular orientations in an electrically poled p(DR1M) homopolymer thin film after a thermal process and several relaxation periods. We have made use not only of the 〈 P1〉 and 〈 P3〉 parameters determined from polarized second-harmonic generation (SHG) measurements, but also of the 〈 P2〉 values extracted from UV-visible spectra and of the 〈 P4〉 values adjusted according to the information entropy theory. In such a thin film with very large nonlinear properties (d33 coefficients were varying from 437.0 to 117.0 pm/V at 1064 nm) it is evidenced that a strong polar order is maintained even after a long relaxation period of 42 days. So, the distribution functions demonstrate that the poling treatment was quite efficient and they emphasize the importance in the determination of both couples of odd and even order parameters in such uniaxially oriented optical elements.


2016 ◽  
Vol 145 (13) ◽  
pp. 134901 ◽  
Author(s):  
Frank Jenz ◽  
Mikhail A. Osipov ◽  
Stefan Jagiella ◽  
Frank Giesselmann

2019 ◽  
Vol 21 (13) ◽  
pp. 6839-6843 ◽  
Author(s):  
Richard J. Mandle ◽  
John W. Goodby

Twist-bend (TB) phases possess a local helical structure with a pitch length of a few nanometers. X-ray scattering experiments on aligned samples of dimeric and oligomeric materials allows the orientational order parameters, orientational distribution functions and heliconical tilt angles to be calculated.


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.


10.12737/6723 ◽  
2014 ◽  
Vol 3 (3) ◽  
pp. 46-56
Author(s):  
Гудкова ◽  
S. Gudkova ◽  
Джумагалиева ◽  
L. Dzhumagalieva ◽  
Еськов ◽  
...  

The present paper shows that the term “complexity” includes absolutely different notions than now it seems to be presented in modern science and philosophy. V.S. Stepin’s postnon-classics has come to this new recognition too close, but, actually, it is a new recognition of uncertainty for systems of the third type (not deterministic and not stochastic). We introduce the interpretation of a type I uncertainty that implies that stochastic methods show systems identified, but methods of the theory of chaos and self-organization and neurocomputing show significant difference of target systems (processes). The concrete examples show the type I uncertainty and give an idea of a type II uncertainty, that implies the coincidence of distribution functions f(x) for different samplings. We prove that neurocomputing method not only differentiates samplings, but also identifies order parameters. In this case we also solve the system synthesis problem.


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