1991
DOI: 10.1364/josab.8.000142
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Birefringent and electro-optic effects in poled polymer films: steady-state and transient properties

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Cited by 170 publications
(62 citation statements)
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“…From Eq. (12), we obtain 4 E(t) =-EpS(t) (15) where S(t) is the Dirac delta function. Substituting Eqs.…”
Section: ) Kt Jmentioning
confidence: 98%
“…From Eq. (12), we obtain 4 E(t) =-EpS(t) (15) where S(t) is the Dirac delta function. Substituting Eqs.…”
Section: ) Kt Jmentioning
confidence: 98%
“…In this paragraph, we show a theoretical model describing the nonlinear optical response of a medium constituted by nonlinear units (chromophores) dispersed in a linear matrix and oriented along a preferential axis [33,34]. We suppose that each molecule is identified by an intrinsic reference system with the axes named 1, 2, 3, and this system can be rotated in respect to the system that describes the whole macroscopic structure with the axes named x, y, z (laboratory axis).…”
Section: Steady-state Properties Of the Induced Electo-optic Coefficientmentioning
confidence: 99%
“…In order to describe these time-dependent phenomena, we introduce the rotational diffusion equation (Smoluchowski-Einstein) for a molecular dipole [33]:…”
Section: Transient Propertiesmentioning
confidence: 99%
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“…In this electret state the polymer manifests a variety of effects: pyroelectricity, piezoelectricity, birefringence, and electro-optical and second-order NLO response. [6][7][8][9][10] All these macroscopic properties of the electret are connected with the microscopic properties of NLO chromophores through the distribution function of chromophores by orientation, because the polarization is never ideal. The properties of the polymer obtained as a result of chromophore orientation may be used for the characterization (and control) of the orientational order of chromophores in the polymer.…”
Section: Introductionmentioning
confidence: 99%