2012
DOI: 10.1016/j.jqsrt.2012.03.026
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Small-angle light scattering and transmittance of polymer film, containing liquid crystal droplets with inhomogeneous boundary conditions

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Cited by 14 publications
(6 citation statements)
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“…n e (x) is the local refractive index for extraordinary wave in point x=x(y,z), n o is the coordinateindependent refractive index for ordinary wave equal to the ordinary refractive index of LC, ⊥ n x Δ is the longitudinal (along the wavevector of incident wave) size of LC droplet elementary volume in which liquid crystal orientation structure is assumed as uniform and determined by only molecular order parameter [7,[22][23][24]…”
Section: Basic Relations To Calculate Small-angle Distribution Of Ligmentioning
confidence: 99%
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“…n e (x) is the local refractive index for extraordinary wave in point x=x(y,z), n o is the coordinateindependent refractive index for ordinary wave equal to the ordinary refractive index of LC, ⊥ n x Δ is the longitudinal (along the wavevector of incident wave) size of LC droplet elementary volume in which liquid crystal orientation structure is assumed as uniform and determined by only molecular order parameter [7,[22][23][24]…”
Section: Basic Relations To Calculate Small-angle Distribution Of Ligmentioning
confidence: 99%
“…(14)- (16), is the extraordinary refractive index of liquid crystal, n x , n y , and n z are the Cartesian components of local director n(r)=(n x , n y , n z ). In case of identical director configuration [7] inside droplets and uniform distribution of LC droplet bipolar axes over the angle, we can write the average components of the vector amplitude scattering function and their squared absolute values (see Eqs. (1) and (2)) as follows: …”
Section: Basic Relations To Calculate Small-angle Distribution Of Ligmentioning
confidence: 99%
See 2 more Smart Citations
“…The effect consists in the fact that in the scattering plane (the plane defined by the wave vectors of the incident and scattered waves) the values of intensities of radiation scattered at angle +θs and angle θs (see Fig.1) are different relative to the illumination direction. Some preliminary data on the effect are given in [29][30][31]. It is worth noting that in films with homogeneous surface anchoring there is a symmetrical distribution of the radiation intensity scattered at the angles +θs and θs [1,2,[29][30][31].…”
Section: Introductionmentioning
confidence: 99%