2000
DOI: 10.1364/ol.25.000832
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Simultaneous optical wavelength interchange with a two-dimensional second-order nonlinear photonic crystal

Abstract: We present a theoretical analysis for simultaneous optical wavelength interchange and isolation of a pair of collinear input optical signals by use of two concurrent difference-frequency-generation processes in a two-dimensional second-order nonlinear photonic crystal. We have derived a set of relations, including a general nonlinear Bragg condition, that we use to determine the parameters of the nonlinear lattice, given the input wavelengths and desired exit angles of the wavelength-interchanged outputs.

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Cited by 57 publications
(29 citation statements)
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“…But this is true under the assumption that the interaction takes place over a very large area compared to the associated wavelengths-that is, for photons with exact momentum. Indeed, this was the regular assumption for the design and analysis of 2-D NPCs [4], [5], [10]. However, allowing (for the realistic) restriction of the interaction width, as exemplified by the use of regular Gaussian beams (or any other finite width beams such as a Bessel beam or a top-hat beam), the photons acquire uncertainty in the transverse direction and phase-matching is possible even if only the longitudinal component of an RLV matches the phase mismatch value.…”
Section: Projection-based Qpmmentioning
confidence: 99%
See 1 more Smart Citation
“…But this is true under the assumption that the interaction takes place over a very large area compared to the associated wavelengths-that is, for photons with exact momentum. Indeed, this was the regular assumption for the design and analysis of 2-D NPCs [4], [5], [10]. However, allowing (for the realistic) restriction of the interaction width, as exemplified by the use of regular Gaussian beams (or any other finite width beams such as a Bessel beam or a top-hat beam), the photons acquire uncertainty in the transverse direction and phase-matching is possible even if only the longitudinal component of an RLV matches the phase mismatch value.…”
Section: Projection-based Qpmmentioning
confidence: 99%
“…3. To find the answer to the equivalent geometrical question we do the following: the numerator and denominator of each of the line parameters are multiplied by a common integer (10) such that they are now relatively prime, that is they have no common divisor except for 1. In other words, their greatest common divisor (gcd) is 1 .…”
Section: B Possibilities For Phase Matchingmentioning
confidence: 99%
“…The phenomenon of wavelength exchanging refers to the simultaneous exchange of power between two signals on different wavelengths [3,13,30]. Wavelength exchanging has been theoretically and experimentally demonstrated using various technologies such as four-wave mixing (FWM) [13,30] and 2-D periodic χ (2) nonlinear photonic crystals [3].…”
Section: Wavelength Exchanging Optical Crossbarmentioning
confidence: 99%
“…Wavelength exchanging has been theoretically and experimentally demonstrated using various technologies such as four-wave mixing (FWM) [13,30] and 2-D periodic χ (2) nonlinear photonic crystals [3]. In [7], different wavelength exchanging technologies are abstracted into a logical device called wavelength exchange optical crossbar (WOC).…”
Section: Wavelength Exchanging Optical Crossbarmentioning
confidence: 99%
“…Both theoretical and experimental results published so far show that this kind of structures can effectively be employed as a host media for realizing many different types of multistep-cascading parametric processes (see, e.g., Broderick, Ross, Offerhaus, Richardson, and Hanna [2000]; Saltiel and Kivshar [2000a]; de Sterke, ; Chowdhury, Hagness, and McCaughan [2000]). Below, we discuss some of the possible application of these 2D structures for multistep parametric interaction and multi-frequency generation.…”
Section: Quadratic 2d Nonlinear Photonic Crystalsmentioning
confidence: 99%