cE11 cE12 cE13 0 0 0 cE 12 cE11 cE13 0 0 0 cE 13 cE13 cE33 0 0 0 0 0 0 cE44 0 0 0 0 0 0 cE 44 0 0 0 0 0 0 cE 66 (A.7) e = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 (A.8) εS = εS xx 0 0 0 εS xx 0 0 0 εSzz (A.9) con cE11 = 26,6 × 1010[N/m2], c33E = 46,99 × 1010[N/m2], cE44 = 12,39 × 1010[N/m2], cE 66 = 18,86 × 1010[N/m2], cE12 = 17,33 × 1010[N/m2], cE13 = 13,62 × 1010[N/m2], εS xx = 89ε0, y εSzz = 173ε0.
Los datos de las constantes fueron tomados de [40].
A.4.
Sulfuro de Cadmio
El rutile (CdS) tiene una densidad ρ = 4820[kg/m3] y forma una estructura cristalina con simetr´ıa hexagonal de clase 6mm, por tanto la matriz de rigidez, la matriz de constantes piezoel´ectricas y la matriz de permitividad el´ectrica tienen la siguiente forma
cE = cE11 cE12 cE13 0 0 0 cE 12 cE11 cE13 0 0 0 cE 13 cE13 cE33 0 0 0 0 0 0 cE44 0 0 0 0 0 0 cE 44 0 0 0 0 0 0 1/2(cE 11− cE12) (A.10) e = 0 0 0 0 ex5 0 0 0 0 ex5 0 0 ez1 ez1 ez3 0 0 0 (A.11)
A.4 Sulfuro de Cadmio 77 εS = εS xx 0 0 0 εSxx 0 0 0 εS zz (A.12) con cE11 = 9,07 × 1010[N/m2], c33E = 9,38 × 1010[N/m2], cE44 = 1,504 × 1010[N/m2], cE 12= 5,81×1010[N/m2], cE13= 5,1×1010[N/m2], ex5 = −0,21[C/m2], ez1= −0,24[C/m2], ez3 = 0,44[C/m2], εSxx = 9,02ε0, y εSzz = 9,53ε0.
78 BIBLIOGRAF´IA
Bibliograf´ıa
[1] Jari-Pascal Curty, Michel Declercq, Catherine Dehollain, and Norbert Joehl. DESIGN AND OPTIMIZATION OF PASSIVE UHF RFID SYS- TEMS . Springer, 2007.
[2] Byunggil Lee and Howon Kim. Design and implementation of a secure ibs platform using rfid and sensor network. In Consumer Electronics, 2006. ISCE ’06. 2006 IEEE Tenth International Symposium on, pages 1–4, 2006.
[3] Xuefeng Jiang and Xu Wang. Study on logistic information acquisition technology in steelmaking practice based on rfid. In Intelligent Control and Automation, 2008. WCICA 2008. 7th World Congress on, pages 7946–7950, 2008.
[4] Guidong Liu, Wensheng Yu, and Yu Liu. Resource management with rfid technology in automatic warehouse system. In Intelligent Robots and Systems, 2006 IEEE/RSJ International Conference on, pages 3706– 3711, 2006.
[5] V. Daniel Hunt, Albert Puglia, and Mike Puglia. RFID: A GUIDE TO RADIO FREQUENCY IDENTIFICATION. Wiley, 2007.
[6] L. Catarinucci, R. Colella, L. Mainetti, V. Mighali, L. Patrono, I. Sergi, and L. Tarricone. An innovative animals tracking system based on passi- ve uhf rfid technology. In Software, Telecommunications and Computer Networks (SoftCOM), 2012 20th International Conference on, pages 1– 7, 2012.
[7] Dong-Beom Shin, Gil young Choi, and Dae-Young Kim. Design and implementation of wireless sensing platform based on uhf rfid techno- logy. In Consumer Electronics (ICCE), 2010 Digest of Technical Papers International Conference on, pages 297–298, 2010.
[8] Miodrag Boli´c and David Simplot-Ryl and Ivan Stojmenovi´c. RFID SYSTEMS. John Wiley & Sons, 2010.
[9] Sanna H¨arm¨a. Surface Acoustic Wave RFID Tags: Ideas, Developments, and Experiments. PhD thesis, Helsinki University of Technology. [10] The global saw tag - a new technical approach to rfid. Technical Report
BIBLIOGRAF´IA 79
[11] V.P. Plessky and L.M. Reindl. Review on saw rfid tags. Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on, 57(3):654– 668, March 2010.
[12] D.E.N. Davies, M.J. Withers, and R.P. Claydon. Passive coded trans- ponder using an acoustic-surface-wave delay line. Electronics Letters, 11(8):163–164, April 1975.
[13] L.M. Reindl and IM. Shrena. Wireless measurement of temperature using surface acoustic waves sensors. Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on, 51(11):1457–1463, Nov 2004. [14] S. H¨arm¨a and V. P. Plessky. Surface acoustic wave rfid tags. In Cristina Turcu, editor, Development and Implementation of RFID Technology. InTech, 2009.
[15] S. Harma, W.G. Arthur, C.S. Hartmann, R.G. Maev, and V.P. Plessky. Inline saw rfid tag using time position and phase encoding. Ultra- sonics, Ferroelectrics and Frequency Control, IEEE Transactions on, 55(8):1840–1846, August 2008.
[16] D.C. Malocha, D. Puccio, and D. Gallagher. Orthogonal frequency co- ding for saw device applications. In Ultrasonics Symposium, 2004 IEEE, volume 2, pages 1082–1085 Vol.2, Aug 2004.
[17] M. Solal and T. Abboud and S. Ballandras and S. Chamaly and V. Laude and R. Lardat and T. Pastureaud and J. Ribbe and W. Steichen and P. Ventura. Fem/bem analysis for saw devices.
[18] O. Nova, N. Pena, and M. Ney. Fdtd simulation of saw rfid tags. In RFID-Technologies and Applications (RFID-TA), 2012 IEEE Interna- tional Conference on, pages 259–262, Nov 2012.
[19] KEN-YA HASHIMOTO and MASATSUNE YAMAGUCHI. Free soft- ware products for simulation and design of surface acoustic wave and surface transverse wave devices. In Frequency Control Symposium, 1996. 50th., Proceedings of the 1996 IEEE International., pages 300–306, Jun 1996.
[20] S. Rahman, H. P. Langtangen, and C. H. W. Barnes. A finite element method for modelling electromechanical wave propagation in anisotropic piezoelectric media. ArXiv Physics e-prints, October 2005.
80 BIBLIOGRAF´IA
[21] Ren´e Marklein. The finite integration technique as a general tool to compute acoustic, electromagnetic, elastodynamic, and coupled wave fields.
[22] P.M. Smith and Wei Ren. Finite-difference time-domain techniques for saw device analysis. In Ultrasonics Symposium, 2002. Proceedings. 2002 IEEE, volume 1, pages 325–328 vol.1, Oct 2002.
[23] King-Yuen Wong and Wai-Yip Tam. Analysis of the frequency response of saw filters using finite-difference time-domain method. Microwave Theory and Techniques, IEEE Transactions on, 53(11):3364–3370, Nov 2005.
[24] F. Chagla and P.M. Smith. Finite difference time domain methods for piezoelectric crystals. Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on, 53(10):1895–1901, October 2006.
[25] Jean-Pierre B´erenger. A perfectly matched layer for the absorption of electromagnetic waves. Journal of Computational Physics, 114(2):185– 200, 1994.
[26] W. C. Chew and Q. H. Liu. Perfectly matched layers for elastodynamics: A new absorbing boundary condition. J. Comp. Acoust, 4:341–359, 1996. [27] A. Taflove and S.C. Hagness. Computational Electrodynamics: The Finite-Difference Time-Domain Method. The Artech House antenna and propagation library. Artech House, Incorporated, 2005.
[28] B. T. Nguyen and S. A. Hutchinson. The implementation of the upwind leapfrog scheme for 3D electromagnetic scattering on massively parallel computers. Technical Report SAND95-1322 UC-705, Sandia National Laboratories (USA), 1995.
[29] W. Yu and R. Mittra. Advanced FDTD Methods: Parallelization, Acce- leration, and Engineering Applications. Artech House electromagnetics series. Artech House, 2011.
[30] Christoph Schr¨oder. On the interaction of elastic waves with buried land mines: An investigation using the finite-difference time-domain method. PhD thesis, Georgia Institute of Technology.
[31] Wolfgang Gentzsch, Lucio Grandinetti, and Gerhard Joubert. High Speed and Large Scale Scientific Computing. IOS Press, 2009.
BIBLIOGRAF´IA 81
[32] Xingjun Zhang, Yanfei Ding, Yiyuan Huang, and Xiaoshe Dong. De- sign and implementation of a heterogeneous high-performance compu- ting framework using dynamic and partial reconfigurable fpgas. In Com- puter and Information Technology (CIT), 2010 IEEE 10th International Conference on, pages 2329–2334, June 2010.
[33] Wenhua Yu. VALU, AVX and GPU Acceleration Techniques for Parallel FDTD Methods. Professional Applications of Computing. Institution of Engineering and Technology, 2013.
[34] Charles Severance. High Performance Computing. Connexions, 2009. [35] D. Royer and E. Dieulesaint. Elastic Waves in Solids I. Springer, 1996. [36] John B. Schneider. Understanding the Finite-Difference Time-Domain
Method. www.eecs.wsu.edu/ schneidj/ufdtd, 2010.
[37] E. Becache, S. Fauqueux, and P. Joly. Stability of perfectly matched layers, group velocities and anisotropic waves, 2003.
[38] K.J. Bathe. Finite Element Procedures. Prentice-Hall International Se- ries in. Prentice Hall, 1996.
[39] Istv´an A. Veres. Stability analysis of second- and fourth-order finite- difference modelling of wave propagation in orthotropic media. Ultraso- nics, 50(3):431 – 438, 2010.
[40] B. A. Auld. Acoustic Fields and Waves in Solids. Robert E. Krieger Publishing Company, 1970.
[41] W. Yu, R. Mittra, T. Su, Y. Liu, and X. Yang. Parallel Finite-Difference Time-Domain Method. Artech House electromagnetics series. Artech House, 2006.
[42] Gen Chen, Lei Zhao, Wen Li, Huadong Zhao, and Yu Wenhua. Per- formance study of avx instructions for the fdtd method. In Cross Strait Quad-Regional Radio Science and Wireless Technology Conferen- ce (CSQRWC), 2013, pages 175–178, July 2013.
[43] Lihong Zhang and Wenhua Yu. Improving parallel fdtd method perfor- mance using sse instructions. In Parallel Architectures, Algorithms and Programming (PAAP), 2011 Fourth International Symposium on, pages 57–59, Dec 2011.
82 BIBLIOGRAF´IA
[44] Agner Fog. Optimizing software in c++. http://www.agner.org/ optimize/, 2004. [Online; accessed 19-April-2014].
[45] J.D. Cooper, A. Valavanis, Z. Ikoni´c, P. Harrison, and J.E. Cunningham. Stable perfectly-matched-layer boundary conditions for finite-difference time-domain simulation of acoustic waves in piezoelectric crystals. Jour- nal of Computational Physics, 253(0):239 – 246, 2013.