Analysis of second harmonic generation in photonic-crystal-assisted waveguides
Author(s) -
A. D’Orazio,
Domenico de Ceglia,
M. De Sario,
Francesco Prudenzano,
Mark J. Bloemer,
M. Scalora
Publication year - 2006
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.2266104
Subject(s) - waveguide , optics , materials science , planar , core (optical fiber) , wavelength , second harmonic generation , scattering , radiation mode , harmonic , signal (programming language) , dielectric , refractive index , optoelectronics , physics , single mode optical fiber , optical fiber , laser , computer graphics (images) , quantum mechanics , computer science , programming language
We study second harmonic generation in a planar dielectric waveguide having alow-index, polymer core layer, bounded by two multilayer stacks. This geometryallows exceptionally strong confinement of the light at the fundamentalwavelength inside the core region with virtually zero net propagation lossesfor distances that exceed several centimeters, provided material and scatteringlosses are neglected. A phase-matched configuration of the waveguide isreported in which the pump signal is the lowest-order mode of the waveguide,and the generated second harmonic signal corresponds to the third propagationmode of the waveguide. Using a polymer waveguide core, having chi(2)=100 pm/V,we predict a conversion efficiency of approximately 90% after a propagationdistance of 2 mm, using peak pump intensities inside the core of the waveguideof 1.35 GW/cm^2. If the waveguide core contains polymer layers with differentglass transition temperatures, the layers can be poled independently tomaximize the overlap integral, and similar pump depletions may be achieved overa distance of approximately 500 microns.Comment: 20 pages, 7 figures, 330k
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