2001
DOI: 10.1070/qe2001v031n01abeh001883
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Telescopic systems with dynamic nonlinear optical correction for distortions

Abstract: This letter deals with the physical interpretation of the 'transitional amplitude' AE, a parameter of percolation theory determined by the derivative mean size of clusters s: AE = x(ds/dx) +s; AE = s( 1 + LR) = where E = xx,, and LR is the average number of red bonds in an incipient infinite cluster.

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Cited by 17 publications
(3 citation statements)
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“…This scheme, demonstrated in Ref. [3], requires two pump beams. What is more, since third-order nonlinearity is weak, the pump powers must be extremely high in order to achieve a reasonably high nonlinear power reflection coefficient, i.e.…”
Section: Introductionmentioning
confidence: 98%
“…This scheme, demonstrated in Ref. [3], requires two pump beams. What is more, since third-order nonlinearity is weak, the pump powers must be extremely high in order to achieve a reasonably high nonlinear power reflection coefficient, i.e.…”
Section: Introductionmentioning
confidence: 98%
“…They also solve the problem of dynamic holographic correction of distortions. [1][2][3][4][5] Thin dynamic holograms formed in an LC layer are free of limitations imposed by angular and spectral selectivities and, therefore, can be used in wide fields of view and a wide spectral range. However, according to the traditional understanding of the mechanism of dynamic grating formation in LC, the fringe of such grating has to have symmetrical profiles.…”
Section: Introductionmentioning
confidence: 99%
“…However, schemes based on thin (plane) dynamic holographic correctors have also been proposed recently [2]. Such schemes are free of the limitations related to spectral and angular selectivity and, therefore, can be used in systems with a large field of view and/or operating with incoherent and nonmonochromatic light.…”
Section: Introduction Thin Dynamic Holograms With An Asymmetric Frinmentioning
confidence: 99%