2018
DOI: 10.1007/s11182-018-1366-x
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Three-Dimensional Model of Holographic Formation of Inhomogeneous PPLC Diffraction Structures

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Cited by 8 publications
(8 citation statements)
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“…Since the changes in the dielectric permittivity tensor of the PSLC (PDLC) sample, caused by the recording processes, are small relative to the unperturbed state [31,32,33,34], it is possible to present the resulting distribution of perturbed dielectric permittivity tensor in the form:for PSLC trueε^(boldnormalr,t)=false(1sans-serifρfalse)[εptrueI^+truem=o,eΔsans-serifε^pm(boldnormalr,t)]+sans-serifρ[sans-serifε^lc+truem=o,eΔsans-serifε^lcm(boldnormalr,t)+Δsans-serifε^lcpolfalse(boldnormalr,tfalse)], for PDLC trueε^(boldnormalr,t)=false(1sans-serifρfalse)[ε…”
Section: Theoretical Modelmentioning
confidence: 99%
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“…Since the changes in the dielectric permittivity tensor of the PSLC (PDLC) sample, caused by the recording processes, are small relative to the unperturbed state [31,32,33,34], it is possible to present the resulting distribution of perturbed dielectric permittivity tensor in the form:for PSLC trueε^(boldnormalr,t)=false(1sans-serifρfalse)[εptrueI^+truem=o,eΔsans-serifε^pm(boldnormalr,t)]+sans-serifρ[sans-serifε^lc+truem=o,eΔsans-serifε^lcm(boldnormalr,t)+Δsans-serifε^lcpolfalse(boldnormalr,tfalse)], for PDLC trueε^(boldnormalr,t)=false(1sans-serifρfalse)[ε…”
Section: Theoretical Modelmentioning
confidence: 99%
“…If in Expression (5), the vectors Ejm are not orthogonal, then in the media a periodic interference pattern will be observed, the intensity distribution of which can be represented as [31]:I(boldnormalr,t)=truem=o,eIm(boldnormalr,t)[1+mm(r)cos(Kmboldnormalr)], where mm(boldnormalr,t)=2I0m(boldnormalr,t)I1m(boldnormalr,t)(e0me1m)/(I0m(boldnormalr,t)+I1m(boldnormalr,t))…”
Section: Theoretical Modelmentioning
confidence: 99%
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