Abstract
An integrated-optical frequency shifter for λ= 1.5µm and a frequency shift of fmod= 6.5GHz has been designed in Ti:LiNbO3 technology. An optical input wave (carrier) at frequency fin is electro-optically converted to an output wave (sideband) at fout = fin ± fmod. Both waves propagate at orthogonal polarizations in the same stripe waveguide. Conversion is effected by an electrical wave of frequency fmod, counter-propagating to the optical waves on a coplanar transmission line. The 3-wave interaction is phase-matched if where Δβ=βc-βs is the waveguide birefringence (βc, βs, propagation constant of carrier and sideband), Ngr is the mean index of optical group velocity, and nel is the ‘effective index’ of the electrical wave. Phase matching is practically achieved by adjustment of the dimensions of the transmission line and of Δβ. In the x-cut, z-propagating LiNbO3 substrate, Δβ could be controlled by adjustment of the width w of the Ti stripe. The birefringence was measured by scanning a polarization coupling perturbation along the waveguide while analyzing the polarization of the output signal [1]. Polarization controllers are applied to the pigtails so that the incident signal can be adjusted to either TE or TM polarization. In this way TE/TM or TM/TE conversion can be selected. Due to the reversal of tire sign of Δβ between these two cases the device operates either as frequency up- or downshifter.
© 1996 IEEE
PDF ArticleMore Like This
R Stolte and R Ulrich
TuD7 International Quantum Electronics Conference (IQEC) 1996
G. Cocorullo, F. G. Della Corte, I. Rendina, A. Rubino, and E. Terzini
ITuB3 Integrated Photonics Research (IPR) 1996
L. M. Johnson, R. A. Becker, and R. H. Kingston
WD4 Integrated and Guided Wave Optics (IGWO) 1984