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Photonic crystals in biology - NanoTR-VI

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Poster Session, Thursday, June 17Theme F686 - N1123Modal Analysis of Circularly Bent Coupled Optical WaveguidesN. Özlem Ünverdi 1* and N. Aydın Ünverdi 21 Department of Electrical-Electronics Eng<strong>in</strong>eer<strong>in</strong>g, Yldz Technical University, stanbul 34349, Turkey2 Department of Mechanical Eng<strong>in</strong>eer<strong>in</strong>g, stanbul Technical University, stanbul 34437, TurkeyAbstract— In this study, a pair of circularly bent, bare, weakly guid<strong>in</strong>g, lossless, multimode and slab optical fibers located <strong>in</strong>the same plane was analyzed. The impact of coupl<strong>in</strong>g on the modal propagation constant was <strong>in</strong>vestigated, and the coupl<strong>in</strong>gbetween even TE leaky modes was found to be stronger than the coupl<strong>in</strong>g between all other leaky modes.Radiation is tangent to the radiation caustic <strong>in</strong> circularly bentoptical waveguides. In this study, the <strong>in</strong>teractions ofevanescent fields of optical waveguides are solved byconsider<strong>in</strong>g the problems of determ<strong>in</strong><strong>in</strong>g the behaviour of<strong>in</strong>cident radiation on a convex surface and modal analysis [1,2].In optics, a beam is an idealized concept of <strong>in</strong>f<strong>in</strong>itesimallyth<strong>in</strong> light cluster. Light beams are modeled as l<strong>in</strong>es <strong>in</strong> physicsand optical problems are solved based on geometricalpr<strong>in</strong>ciples. In this study, a pair of circularly bent, bare, weaklyguid<strong>in</strong>g, lossless, multimode and slab optical waveguideswhich are surrounded by a simple medium as shown <strong>in</strong> Figure1, are considered as scatter<strong>in</strong>g objects, and the effect of one ofthe waveguide’s radiation on the other waveguide’s behaviouris exam<strong>in</strong>ed by Geometric Theory of Diffraction (GTD) whichexpla<strong>in</strong>s the diffraction of very high frequency waves byasymptotic methods [3-6].utilized by consider<strong>in</strong>g the propagation directions of theoptical waveguides. It is obvious that, the coupled bare andslab optical waveguides considered <strong>in</strong> this study must be <strong>in</strong> thesame plane.In the analysis, the effective regions of optical waveguides <strong>in</strong>mutual coupl<strong>in</strong>g, which are amongst the important parametersof optical directional couplers, are determ<strong>in</strong>ed. It is observedthat the effected region of one of the circularly bent coupledoptical waveguides by the other optical waveguide is equal tothe longer arc length between the po<strong>in</strong>ts of common <strong>in</strong>ner andouter tangents on the radiation caustic. On the other hand, theeffected region of the other waveguide by this waveguide isequal to the shorter arc length. It is concluded that the aboveobservations are <strong>in</strong>dependent of the propagation directions, <strong>in</strong>other words, of the feed<strong>in</strong>g directions of the opticalwaveguides.In this study, <strong>in</strong> TE and TM leaky modes of opticalwaveguides, the variation <strong>in</strong> the modal propagation constantbecause of coupl<strong>in</strong>g is <strong>in</strong>vestigated. As a result of the analysis,it is proved that the coupl<strong>in</strong>g between even TE leaky modes ismore efficient than those amongst the other modes. As anatural consequence of coupl<strong>in</strong>g mechanism, it is observedthat the coupl<strong>in</strong>g amongst the leaky modes and radiationmodes is stronger than those amongst the evanescent fields ofthe guided modes.The authors express their s<strong>in</strong>cere gratitudes to Dr. S. ÖzenÜnverdi for helpful discussions and suggestions.*unverdi@yildiz.edu.trFigure 1. A pair of circularly bent, bare and slab optical waveguides.The path of the light beam on the optical waveguide isdeterm<strong>in</strong>ed by Fermat pr<strong>in</strong>ciple. In this study, it is assumedthat there are not s<strong>in</strong>gular po<strong>in</strong>ts on the surfaces of theanalyzed optical waveguides, all the surface po<strong>in</strong>ts areconsidered as regular. In spite of the fact that, accord<strong>in</strong>g to theGeneral Relativity Theory, the light beams pass<strong>in</strong>g nearby theoptical waveguide without hitt<strong>in</strong>g it are bent towards thewaveguide, the present coupl<strong>in</strong>g analysis neglects this effect.In circularly bent optical waveguides, the radiation is <strong>in</strong> fact<strong>in</strong>side the beam tube. However, <strong>in</strong> this study, where the mutualcoupl<strong>in</strong>g mechanism of optical waveguides is analyzed andeffective lengths are determ<strong>in</strong>ed, the aforementioned beamtube is considered as a s<strong>in</strong>gle beam. In determ<strong>in</strong><strong>in</strong>g theeffected region of an optical waveguide by the radiation of theother waveguide and the effective region of the radiat<strong>in</strong>goptical waveguide <strong>in</strong> the coupl<strong>in</strong>g phenomena, the “common<strong>in</strong>ternal tangent” and “common external tangent” concepts are[1] A. W. Snyder and J. D. Love, Optical Waveguide Theory, J. W.Arrowsmith Ltd., Bristol - Great Brita<strong>in</strong>, 1983.[2] N. Ö. Ünverdi, “The Effect of Evanescent Fields of GuidedModes and Leaky Modes on Mutual Coupl<strong>in</strong>g of Straight and BentOptical Waveguides”, Ph.D. Thesis, Yıldız Technical University,Istanbul, Turkey, 1998.[3] W. H. Louisell, Coupled Mode Parametric Electronics, JohnWiley & Sons, New York, 1960.[4] C. A. Balanis, Advanced Eng<strong>in</strong>eer<strong>in</strong>g Electromagnetics, JohnWiley & Sons Inc., New York, 1989.[5] J. M. Senior, Optical Fiber Communications, Second Edition,Prentice-Hall, Cambridge, 1992.[6] M. N. O. Sadiku, Optical and Wireless Communications, CRCPress, New York, 2002.6th Nanoscience and Nanotechnology Conference, zmir, 2010 629

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