2000
DOI: 10.1103/physrevlett.85.1863
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Diffraction Management

Abstract: By using the diffraction properties of waveguide arrays, we propose a scheme to produce structures with designed diffraction. We fabricated arrays with reduced, canceled, and even reversed diffraction. Results of experiments with such waveguides are presented and compared with the predictions made by coupled-mode theory.

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Cited by 519 publications
(410 citation statements)
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“…The result of this check is summarized in Fig.4.c where a clear separation of the central peaks of the pulses is visible in propagation, while the shapes of the individual pulses distort negligibly. , by solving numerically (7). We note that the fringes appear both in the initial superposition pattern as well as in propagated pattern, which is due to nonuniform phases of the constituent pulses.…”
Section: Fig2mentioning
confidence: 96%
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“…The result of this check is summarized in Fig.4.c where a clear separation of the central peaks of the pulses is visible in propagation, while the shapes of the individual pulses distort negligibly. , by solving numerically (7). We note that the fringes appear both in the initial superposition pattern as well as in propagated pattern, which is due to nonuniform phases of the constituent pulses.…”
Section: Fig2mentioning
confidence: 96%
“…We searched for particular spatio-temporal shapes of the pulses which are invariant under the propagation described by (7). The pulse propagating invariantly with the group velocity 1 V is obtained directly from (6):…”
Section: Fig2mentioning
confidence: 99%
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“…A great deal of attention has also been recently attracted to more special cases, when the diffraction is subject to various forms of management, so that the diffraction coefficient gradually vanishes or periodically changes its sign [1]. In particular, it was shown in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…In the most typical experimental situation, with the power of light beams 500 − 1000 W, the nonlinearity length in AlGaAs waveguides (whose nonlinearity is 500 time stronger than that of fused silica glass) takes values ∼ 1 − 2 mm, and the coupling length is ∼ 1 mm [11,12]. In fact, L coupl may vary in broad limits, as it exponentially depends on the separation h between the waveguides: for instance, L coupl decreases by a factor of 1.6 as h increases from 9 µm to 11 µm [11].…”
Section: Introductionmentioning
confidence: 99%