“…The first term in this trial function represents a varying nematicon-like beam, while the second term represents the diffractive radiation of low wavenumber which accumulates under the evolving nematicon [27,31]. This radiation cannot remain flat, so it is assumed that g is non-zero in the interval −ℓ/2 ≤ y ≤ ℓ/2 [27,31]. Substituting the optical field form (4) into the director equation, the second of (2), and using the one space dimensional boundary condition θ = 0 at the cell walls y = ±L gives the solution…”