Order parameters

The uniaxial order parameter is zero for an isotropic fluid and one for a perfectly aligned system. First one calculates a director vector (see Ref. 2)

$Q_{\alpha \beta }=\frac{1}{N}\sum _{j=1}^N(\frac{3}{2}{\hat{e}}_{j\alpha }{\hat{e}}_{j\beta }-\frac{1}{2}{\delta }_{\alpha \beta }),\alpha ,\beta =x,y,z,$

where $Q$ is a second rank tensor, ${\hat{e}}_j$ is a unit vector along the molecular long axis, and ${\delta }_{\alpha \beta }$ is the Kronecker delta. Diagonalisation of this tensor gives three eigenvalues ${\lambda }_{+}$, ${\lambda }_0$ and ${\lambda }_{-}$, and $n$ is the eigenvector associated with the largest eigenvalue (${\lambda }_{+}$). From this director vector the nematic order parameter is calculated from (see Ref. 3)

$S_2={\lambda }_{+}=⟨P_2(n\cdot e)⟩=⟨P_2(\cos \theta )⟩=⟨\frac{3}{2}{\cos }^2\theta -\frac{1}{2}⟩$

where $S_2$ is known as the uniaxial order parameter. Here $P_2$ is the second order Legendre polynomial, $\theta$ is the angle between a molecular axes and the director $n$, and the angle brackets indicate an ensemble average.

References

1. Joseph P. Straley "Ordered phases of a liquid of biaxial particles", Physical Review A 10 pp. 1881 - 1887 (1974)
2. R. Eppenga and D. Frenkel "Monte Carlo study of the isotropic and nematic phases of infinitely thin hard platelets", Molecular Physics 52 pp. 1303-1334 (1984)
3. Mark R. Wilson "Determination of order parameters in realistic atom-based models of liquid crystal systems", Journal of Molecular Liquids 68 pp. 23-31 (1996)
4. Denis Merlet, James W. Emsley, Philippe Lesot and Jacques Courtieu "The relationship between molecular symmetry and second-rank orientational order parameters for molecules in chiral liquid crystalline solvents", Journal of Chemical Physics 111 pp. 6890-6896 (1999)