• Acta Photonica Sinica
  • Vol. 34, Issue 4, 537 (2005)
[in Chinese], [in Chinese], [in Chinese], [in Chinese], and [in Chinese]
Author Affiliations
  • [in Chinese]
  • show less
    DOI: Cite this Article
    [in Chinese], [in Chinese], [in Chinese], [in Chinese], [in Chinese]. Boundary Condition and Initial Condition in the Time-domain Beam Propagation Methods Applied to Study Planar Waveguides[J]. Acta Photonica Sinica, 2005, 34(4): 537 Copy Citation Text show less
    References

    [1] Eldada L. Telecom optical componentry: past, present, future.Proceedings of SPIE , 2001,4604:1 ~ 15

    [2] Tao Z H, Chang J H, Sun X H, et al. A novel design method for broadband fiber raman amplifier. Acta Photonica Sinica,2004,33(4) :435~438

    [3] Li C Q,Sun X H,Zhang M D,et al. Configuration research of 2D-OOC signature sequence code for OCDMA system. Acta Photonica Sinica, 2003,32 (1) :46 ~ 50

    [4] Li C Q,Sun X H,Zhang M D,et al. Configuration research of 2D-RSC signature sequence code for OCDMA system. Acta Photonica Sinica, 2004,33(2): 187 ~ 191

    [5] Chu S T. Modeling of guided-wave optical structures by the finite-difference time-domain method. [ Ph. D. dissertion ] ,University of Waterloo, Waterloo, Ont., Canada,1990

    [6] Yevick D. A guide to electric field propagation techniques for guided-wave optics. Opt. Quantum Electron, 1994,26:S185~S197

    [7] Liu P L, Zhao Q,Choa F S. Slow-wave finite-difference beam propagation method. IEEE Photon Technol Lett, 1995,7(9) :890~892

    [8] Ma F. Slowly varying envelope simulation of optical waves in time domain with transparent and absorbing boundary conditions. J Lightwave Technol, 1997,15 (10): 1974 ~ 1985

    [9] Hadley G R. Transparent boundary condition for the beam propagation method. Opt Lett, 1991,16 (9) :624 ~ 626

    [10] Higdon R L. Absorbing boundary condition for difference approximation to the multidimensional wave equation. Math Comput, 1986,47(176): 437~459

    [11] Ramahi O M. Complementary operators: A method to annihilate artificial reflections arising from the truncation of the computational domain in the solution of partial difference equations. IEEE Trans Antennas Propagat,1995,43(14) :697 ~704

    [12] Berenger J P. A perfectly matched layer for the absorption of electromagnetic waves. J Comput Phys, 1994,114 (2): 185~200

    [13] Yamauchi J, Shibayama J, Sekiguchi M, et al. Finitedifference beam propagation method based on the generalized Douglas scheme for a nonuniform grid. IEEE Photon Technol Lett, 1997,9(1) :67~69

    [14] Yamauchi J, Shibayama J,Sainto O,et al. Improved finitedifference beam propagation method based on the generalized Douglas scheme and its application to semivectorial analysis. J Lightwave Technol, 1996, 14(10) :2401~ 2406

    [16] Shibayama J, Takahashi T, Yamauchi J, et al. Efficient time-domain finite-difference beam propagation method for the analysis of slab and circularly symmetric waveguides. J Lightwave Technol, 2000,18(3) :437~442

    [17] Shibayama J,Takahashi T, Yamauchi J, et al. Comparative study of absorbing boundary condition for the time-domain beam propagation method. IEEE Photon Technol Lett,2001,13(4): 314 ~316

    [18] Yamauchi J, Shibayama J, Nakano H. Application of the generalized Douglas scheme to optical waveguide analysis.Opt Quantum Electron, 1999,31(4) :675~687

    CLP Journals

    [1] HUANG Yao, HUANG Xu-guang, HU She-jun. A Planar-Lightwave-Circuit Triplexer[J]. Acta Photonica Sinica, 2009, 38(1): 39

    [in Chinese], [in Chinese], [in Chinese], [in Chinese], [in Chinese]. Boundary Condition and Initial Condition in the Time-domain Beam Propagation Methods Applied to Study Planar Waveguides[J]. Acta Photonica Sinica, 2005, 34(4): 537
    Download Citation