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1. 2. 3. 4. © 3-D Full-Vectorial Analysis Of Strong Optical Waveguide Discontinuities Using Pade Approximants Jamid, HA; Khan, MZM IEEE-INST ELECTRICAL.

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Presentation on theme: "1. 2. 3. 4. © 3-D Full-Vectorial Analysis Of Strong Optical Waveguide Discontinuities Using Pade Approximants Jamid, HA; Khan, MZM IEEE-INST ELECTRICAL."— Presentation transcript:

1 1. 2. 3. 4. © 3-D Full-Vectorial Analysis Of Strong Optical Waveguide Discontinuities Using Pade Approximants Jamid, HA; Khan, MZM IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC, IEEE JOURNAL OF QUANTUM ELECTRONICS; pp: 343-349; Vol: 43 King Fahd University of Petroleum & Minerals http://www.kfupm.edu.sa Summary A full-vectorial 3-D numerical method applicable to high-index contrast optical waveguide discontinuities is presented. Rigorous treatment of the longitudinal boundary condition is incorporated in the, formulation. The square root of the characteristic matrix is approximated using Pade approximants which results in an efficient implementation. The biconjugate gradient stabilized method is utilized to iteratively calculate the reflected and transmitted fields. A preconditioner is proposed which results in reduced number of iterations. The proposed method is applied to various optical waveguide facets exhibiting strong transverse and longitudinal refractive index discontinuities. In all cases, the modal reflectivities of the fundamental TE-Like and TM-Like modes are calculated for both the full-vectorial and the semi-vectorial formulations. Significant difference in the calculated modal reflectivity is seen between the full and semi-vectorial models. The error in the power balance remains low in the full-vectorial case irrespective of the waveguide dimensions. However, in the semi-vectorial case, the error in the power balance is found to increase when the waveguide width is reduced. References: BIERWIRTH K, 1986, IEEE T MICROW THEORY, V34, P1104 BURTON RS, 1994, ELECTRON LETT, V30, P1071 CHIOU YP, 1997, IEEE PHOTONIC TECH L, V9, P964 ELREFAEI H, 2000, IEEE PHOTONIC TECH L, V12, P158 Copyright: King Fahd University of Petroleum & Minerals; http://www.kfupm.edu.sa

2 5. 6. 7. 8. 9. 10. 12. 13. 14. 15. 16. 17. 19. 20. 22. 24. 25. 26. 27. 28. 29. 30. 31. 32. 33. 34. © ELREFAEI H, 2000, IEEE PHOTONIC TECH L, V12, P389 FENG NN, 2003, IEEE J QUANTUM ELECT, V39, P1661, DOI 10.1109/JQE.2003.819555 FENG NN, 2003, J LIGHTWAVE TECHNOL, V21, P1996, DOI 10.1109/JLT.2003.816892 FENG NN, 2004, IEEE PHOTONIC TECH L, V16, P461, DOI 11. 18. 21. 23. 10.1109/LPT.2003.821245 GERDES J, 1995, ELECTRON LETT, V31, P65 HERZINGER CM, 1993, IEEE J QUANTUM ELECT, V29, P2273 HO PL, 2001, IEEE PHOTONIC TECH L, V13, P1316 JAMID HA, 2004, IEEE T MICROW THEORY, V52, P1166, DOI 10.1109/TMTT.2004.825643 JIANG K, 2005, J LIGHTWAVE TECHNOL, V23, P4239, DOI 10.1109/JLT.2005.858227 KAWANO K, 1998, IEEE PHOTONIC TECH L, V10, P108 LU YY, 2002, IEEE PHOTONIC TECH L, V14, P1533, DOI 10.1109/LPT.2002.803904 OBAYYA SSA, 2004, J LIGHTWAVE TECHNOL, V22, P1420, DOI 10.1109/JLT.2004.827671 RAHMAN BMA, 1988, J LIGHTWAVE TECHNOL, V6, P52 RAO H, 1999, IEEE PHOTONIC TECH L, V7, P830 RAO HL, 2000, J LIGHTWAVE TECHNOL, V18, P1155 REED M, 1998, IEE P-OPTOELECTRON, V145, P53 ROGGE U, 1993, J LIGHTWAVE TECHNOL, V11, P2015 ROZZI T, 1992, IEEE T MICROW THEORY, V40, P1879 SCHUBERT P, 1994, J MUSICOLOGY, V12, P3 SMARTT CJ, 1993, ELECTRON LETT, V29, P1352 SZTEFKA G, 1993, IEEE PHOTONIC TECH L, V5, P554 VIELVA LA, 1994, P MICROW ANTENNAS PR, V141, P127 WEI SH, 2002, IEEE PHOTONIC TECH L, V14, P645 For pre-prints please write to: hajamed@kfupm.edu.sa; zahedmk@yahoo.co.in Copyright: King Fahd University of Petroleum & Minerals; http://www.kfupm.edu.sa


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