1987
DOI: 10.1364/josab.4.000968
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Second-order nonlinear-optical processes in orientationally ordered materials: relationship between molecular and macroscopic properties

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Cited by 566 publications
(223 citation statements)
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“…Before further proceeding, it is emphasized that the theoretical framework presented in this work parallels the theory of dye-doped polymers, called Singer-Kuzyk-Sohn (SKS) model of electric poling, 56 which includes the effects of local potentials U n (Ω, F) due to applied poling field. Singer et al 56 showed that liquid crystals and polymer glasses can be formed into orientationally ordered materials by raising the temperature of the material at which molecular motion is greatly enhanced, applying an external aligning field and then cooling with the field applied. SKS model is a sort of nonlinear optical version of the Maier-Saupe model 57 of liquid crystal phase to describe the electric field poling of dye-doped polymers.…”
Section: Molecular Orientational Contributions To Nonlinear Macrmentioning
confidence: 99%
See 1 more Smart Citation
“…Before further proceeding, it is emphasized that the theoretical framework presented in this work parallels the theory of dye-doped polymers, called Singer-Kuzyk-Sohn (SKS) model of electric poling, 56 which includes the effects of local potentials U n (Ω, F) due to applied poling field. Singer et al 56 showed that liquid crystals and polymer glasses can be formed into orientationally ordered materials by raising the temperature of the material at which molecular motion is greatly enhanced, applying an external aligning field and then cooling with the field applied. SKS model is a sort of nonlinear optical version of the Maier-Saupe model 57 of liquid crystal phase to describe the electric field poling of dye-doped polymers.…”
Section: Molecular Orientational Contributions To Nonlinear Macrmentioning
confidence: 99%
“…(A12) and Eq. (A17) we have (56) from which the nonvanishing components for αα(−ω; ω, 0, 0) class are αα iiii , αα iijj and αα ijji for i j ∈ {X, Y, Z }, where αα iijj = αα jjii and αα ijij = αα jiji = αα ijji = αα jiij with the isotropic condition αα iiii = αα iijj + 2 αα ijij . Similar relations for ᾱ µµ(−ω; ω, 0, 0) class may be expressed as in αα(−ω; ω, 0, 0) class, replacing α JK (0) and α KK (0) by µ J µ K and µ K µ K (= µ · µ), respectively.…”
Section: Quadratic Electro-optic (Or DC Kerr) Effectmentioning
confidence: 99%
“…( ) where ε r0 is the static relative dielectric constant and ε r∞ is the relative dielectric constant in the range of optical frequencies [12,23]. The main characteristics are reported in Table 1 [12,[24][25][26][27][28][29].…”
Section: Electro-optic Properties Of a Single Moleculementioning
confidence: 99%
“…In such a technique [23] it is not necessary to apply electrodes on the polymeric material, as a consequence, it is possible for example to deposit, by spin coating, a polymeric film directly on a bare substrate. In the corona poling procedure the sample is put on a metal plate that plays simultaneously the role of heater and bottom electrode.…”
Section: Inducing Of the Macroscopic Electro-optic Propertiesmentioning
confidence: 99%
“…Under the condition of pp-polarization in addition to the assumptions that the Kleinman symmetry 63 is satisfied and that the axis of anisotropy is perpendicular to the sample surface with C v symmetry, 64 the effective SHG coefficient is written as follows:…”
mentioning
confidence: 99%