1999
DOI: 10.1364/ol.24.000896
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Quasi-phase-matched difference-frequency generation in periodically poled Ti:LiNbO_3 channel waveguides

Abstract: Mid-infrared radiation near 2.8 mum was generated by difference-frequency generation in an 80-mm-long periodically poled Ti:LiNbO(3) channel waveguide by pump radiation near 1.55 mum (tunable external-cavity laser) and a signal radiation of 3.391 mum (HeNe laser). We obtained a normalized conversion efficiency of 105% W(-1) , which is to our knowledge the highest value ever reported.

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Cited by 66 publications
(22 citation statements)
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“…Enhancement of the mid-infrared output power in DFG by use of optical amplifiers, build-up cavities, or laser intracavity DFG typically increases the system cost and complexity, which is disadvantageous in field applications of molecular spectroscopy. Difference-frequency generation in a quasiphase-matched waveguide nonlinear crystal, on the other hand, is an elegant solution to increase the output power without adding much to system cost, size, or complexity [34,42,43,44,45]. A waveguide fabricated in the crystal concentrates the input laser fields in a small mode area of approximately 100 µm 2 .…”
Section: Typical Implementationsmentioning
confidence: 99%
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“…Enhancement of the mid-infrared output power in DFG by use of optical amplifiers, build-up cavities, or laser intracavity DFG typically increases the system cost and complexity, which is disadvantageous in field applications of molecular spectroscopy. Difference-frequency generation in a quasiphase-matched waveguide nonlinear crystal, on the other hand, is an elegant solution to increase the output power without adding much to system cost, size, or complexity [34,42,43,44,45]. A waveguide fabricated in the crystal concentrates the input laser fields in a small mode area of approximately 100 µm 2 .…”
Section: Typical Implementationsmentioning
confidence: 99%
“…Use of a chirped or apodized QPM instead of a uniform QPM structure reduces the output power by an order of magnitude, but provides a wavelength tuning range of tens of nanometres with a single waveguide, without the need to change the crystal temperature [34]. The input beams can be coupled into the waveguide in free space, by tightly focusing the beams into the input aperture of the waveguide [44]. However, owing to the small size of the aperture, fibre coupling is often a more convenient and reliable solution, especially in field applications [34].…”
Section: Typical Implementationsmentioning
confidence: 99%
“…Since the Tiindiffusion process temperature is high, the QPM structure must be formed after the waveguide preparation. A related problem is that an unwanted domain-inverted layer of ∼ 50 μm thickness is formed on the initial +Z surface by Li 2 O outdiffusion during the Ti-indiffusion process, disabling the domain inversion [115]. The QPM structures are formed by removing the unwanted domain-inverted layer by polishing, uniform domain inversion, and applying a voltage pulse through a periodic electrode.…”
Section: Device Fabricationmentioning
confidence: 99%
“…When a continuous input wave is used, the efficiency can be improved by increasing the interaction length. There have been many publications on highly efficient LiNbO 3 (LN) second-order nonlinear optic wavelength conversion devices [2][3][4].…”
Section: Introductionmentioning
confidence: 99%