2000
DOI: 10.1109/68.817501
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Efficient wide-band and tunable midspan spectral inverter using cascaded nonlinearities in LiNbO3 waveguides

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Cited by 73 publications
(22 citation statements)
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“…Its excellent electro-optical and nonlinear optical properties are exploited in various applications such as: laser frequency doublers, wideband tunable light sources, light amplification, quasi-phase-matched frequency convertors, surface acoustic waves, optical switches and modulators, multiplexors and for many other all-optical signals processing. Most of the integrated optics devices designed for these applications are based on waveguides fabricated either by Ti-indiffusion [1,2] or by one of the proton exchange techniques namely Annealed Proton Exchange (APE) [3][4][5], Reverse Proton Exchange (RPE) [6] or Soft Proton Exchange (SPE) [7][8][9][10]. All these techniques allow fabricating low loss waveguides with preserved electro-optical and nonlinear properties, but in return lead to low refractive index increase typically in the range of ∆n e =0.01 for Tiindiffusion [11], ∆n e =0.02 for APE and RPE [6] and ∆n e =0.03 for SPE [7].…”
Section: Introductionmentioning
confidence: 99%
“…Its excellent electro-optical and nonlinear optical properties are exploited in various applications such as: laser frequency doublers, wideband tunable light sources, light amplification, quasi-phase-matched frequency convertors, surface acoustic waves, optical switches and modulators, multiplexors and for many other all-optical signals processing. Most of the integrated optics devices designed for these applications are based on waveguides fabricated either by Ti-indiffusion [1,2] or by one of the proton exchange techniques namely Annealed Proton Exchange (APE) [3][4][5], Reverse Proton Exchange (RPE) [6] or Soft Proton Exchange (SPE) [7][8][9][10]. All these techniques allow fabricating low loss waveguides with preserved electro-optical and nonlinear properties, but in return lead to low refractive index increase typically in the range of ∆n e =0.01 for Tiindiffusion [11], ∆n e =0.02 for APE and RPE [6] and ∆n e =0.03 for SPE [7].…”
Section: Introductionmentioning
confidence: 99%
“…The multitude of offangle reciprocal vectors makes possible either multi-wavelength parametric generation and amplification or the emission of the same generated wavelength in more than one direction. These possibilities may find potentially interesting applications in, for example, simultaneous multiple-trace-gas detection [4] where several wavelengths are required at the same time or in multichannel information processing where efficient cascaded conversion of several wavelengths are necessary [5]. However, parametric generation and amplification in a 2D NPC has not been reported even though 1D NPC QPM optical parametric oscillators (OPOs) were demonstrated from the early days of periodic poling for QPM [6].…”
Section: Introductionmentioning
confidence: 99%
“…Thus, conversion is realized in which the input/output waves stay in the same wavelength band and high-speed switching of the DF wave is realized by the pump wave. Many publications have dealt with this point [12,13].…”
Section: Cascaded Shg/dfgmentioning
confidence: 99%