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Performance advantages of CPML over UPML absorbing boundary conditions in FDTD algorithm

References [1] J. P. Berenger, ”A Perfectly Matched Layer for the Absorption of Electromagnetic Waves”, Journal of Computational Physics, vol.114, pp.185-200, 1994. [2] Z. S. Sacks, D. M. Kingsland, R. Lee and J. F. Lee, ”A Per- fectly Matched Anisotropic Absorber for Use as an Absorbing Boundary Condition”, IEEE Trans. Antennas Propagat., vol. 43, 1460-1463, 1995. [3] S. D. Gedney, ”An Anisotropic Perfectly Matched Layer Absorb- ing Media for the Truncation of FDTD Lattices”, IEEE Trans. Antennas Propagat., vol

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On Some Strategies for Computer Simulation of Thewave Propagation Using Finite Differences II. Multi–Dimensional FDTD Method

References [1] ŠUMICHRAST,. : On Some Strategies for Computer Simulation of the Wave Propagation using Finite Differences, I. One-Dimensional FDTD Method, J. Electrical Engineering 64 No. 4 (2013), 212-221. [2] YEE, K. S. : Numerical Solution of Initial Boundary Value Problems Involving Maxwell’s Equations in Isotropic Media, IEEE Trans. on Antennas and Prop. AP-14 No. 3, (1966), 302-307. [3] BI, Z.-WU, K.-WU, C.-LITVA, J. : A New Finite-Difference Time-Domain Algorithm for Solving Maxwell’s Equations

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SHI irradiation induced modifications of plasmonic properties of Ag-TiO2 thin film and study using FDTD simulation

, 5, (2015), 1265. [30] . [31] H agemann H.J., G udat W., K unz C., J. Opt. Soc. Am., 65, (1975), 742. [32] L ink S.S., E l -S ayed M.A., Int. Rev. Phys. Chem., 19, (2000), 409.

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On Some Strategies for Computer Simulation of the Wave Propagation Using Finite Differences I. One–Dimensional FDTD Method

Some strategies used in the computer simulation of wave phenomena by means of finite differences in time-domain (FDTD) method are reviewed and discussed here. It is shown that the wave equation in its discretized form possesses different properties in comparison with the true differential formulation. In this part the issues of stability and numerical dispersion are thoroughly investigated for the one-dimensional case represented here by waves on transmission lines and transversal electromagnetic plane wave

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A New Design of Metamaterials for SAR Reduction

., Fujiwara, O. (1999). FDTD computation of temperature rise in the human head for portable telephones. IEEE Transactions on Microwave Theory and Techniques , 47 (8), 1528-1534. [18] Islam, M.T., Faruque, M.R.I., Misran, N. (2009). Design analysis of ferrite sheet attachment for SAR reduction in human head. Progress in Electromagnetics Research (PIER) , 98, 191-205. [19] Kuo, C.M. (2003). SAR distribution and temperature increase in the human head for mobile communication. In IEEE Antennas and Propagation Society International Symposium

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Numerical Analysis of Transmission Lines Equation by new β-method Schemes

References [1] David B. Davidson, Computational Electromagnetics for RF for RF and Microwave Engineering Second Cambridge university Press, 2011. [2] J. Clerk Maxwell, A Treatise on Electricity and Magnetism, 3rd ed., vol. 2. Oxford: Clarendon, 1892, pp.68-73. [3] Erturk E, Corke TC, Gokcol C.numerical solutions of 2- D steady in- compressible driven cavity ow at high Reynolds numbers. International journal for Numerical Methods in uids 2005; 48:747-774. [4] S. Zhao and G.W. Wei, High-order FDTD

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On Some Aspects of the Complex–Envelope Finite–Differences Simulation of Wave Propagation in One–Dimensional Case

Computer Simulation of the Wave Propagation using Finite Differences I., One-dimensional FDTD method, JEEEC 64 No. 4 (2013), 212-221. [5] ŠUMICHRAST, L’. : On Some Strategies for Computer Simulation of the Wave Propagation using Finite Differences II. Multi-Dimensional FDTD Method, J. Electrical Engineering 64 No. 6 (2013), 337-345. [6] CHANGNING MA-ZHIZHANG CHEN: Stability Analysis of the CE-FDTD Method, IEEE Microwave & Wireless Comp. Lett. 14 No. 5 (2004), 243

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Tapered fiber sensor in the near infrared wavelength


Simulated transmission spectra for tapered fibers with no taper, one taper and two tapers in the near infrared wavelength range, calculated by Finite-Difference-Time-Domain method are currently presented. Transmission peak positions tend to shift to the shorter wavelength when the taper deformation is added to the fiber or the taper width gets narrower. The thickness sensitivity for the tapered structures with different taper thicknesses is about 2.28e-3 nm·µm−1. There is an interference structure in the electric field distribution images, which reveals in the fiber structures. The transmission spectra for the fiber without taper, one taper and two-tapered structures were simulated in near infrared wavelength by FDTD. The transmission spectra for tlated in near infrared wavelength by FDTD. The sensitivity of the fiber was about 50 nm × RIU−1 and it had better refractive index detection. The tapered fiber can be applied to the bio-chemical sensors and physical deformation testing.

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Aperture Coupled Microstrip Short Backfire Antenna

.—SIMON, P.: Microstrip Backfire Antenna, Proceedings IEEE AP-S Symposium, 1981, pp. 343-346. BALANIS, C. A.: Modern Antenna Handbook, A John Wiley & Sons, Inc., 2008. LEE, R. Q.—LEE, K. F.: Experimental Study of the Two-Layer Electromagnetically Coupled Rectangular Patch Antenna, IEEE Trans. on AP 38 No. 8 (1990), 1298-1302. NISHIYAMA, E.—AIKAWA, M.: FDTD Analysis of Stacked Microstrip Antenna with High Gain, Progress In Electromagnetics Research, PIER 33 (2001), 29

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Comparative Electromagnetic and Quasi–Static Simulations of a Shortpulse Propagation along Microstrip Meander Delay Lines with Design Constraints

, A. U.—HOLLOWAY, C. L.—PIKET-MAY, M. : Meander Delay Line Challenge Problem: a Comparison using FDTD, FEM and MoM, 2001 IEEE EMC Int. Symp. Symp. Rec. Int. Symp. Electromagn. Compat. (Cat. No.01CH37161), vol. 2, 2001, doi:10.1109/ISEMC.2001.950479. [8] The Finite Integration Technique, (n.d.). . [9] GAZIZOV, T. R. : Analytic Expressions for MOM Calculation of Capacitance Matrix of Two Dimensional System of conductors and Dielectrics Having Arbitrarily Oriented Boundaries, 2001 IEEE EMC Int. Symp. Symp. Rec. Int

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