Finite element calculation of the dispersion relations of infinitely extended SAW structures including bulk wave radiation

In the design procedure of surface acoustic wave (SAW) devices simple models like equivalent circuit models or the Coupling of Modes (COM) model are used to achieve short calculation times. Therefore, these models can be used for iterative component optimization. However, they are subject to many simplifications and restrictions. In order to improve the parameters required for the simpler models and to achieve better insight ot the physics of SAW devices analysis tools solving the constitutional partial differential equations are needed. We have developed an efficient calculation scheme based on the finite element method. It makes use of newly established periodic boundary conditions (PBCs) allowing the simulation of an infinitely extended SAW device. This is a good approximation of many SAW devices which show a large number of periodically arranged electrodes. We have developed two different formulations for the PBCs: One leads to a small quadratic eigenvalue problem operating on a larger matrix. These formulations allow the calculation of the complete dispersion relation. Bulk acoustic waves (BAWs) which are generated due to mode conversion at electrode edges are allowed to leave the calculation area nearly without reflection. Therefore, the calculation scheme also considers damping coefficients caused by the conversion of surface waves into bulk waves. This behavior coincides well with real SAW devices in which the substrate thickness is large compared to the used wavelengths and, additionally, the bulk waves are scattered in all directions at the rough substrate bottom. In the paper, a short introduction to the basic theory of the numerical calculation scheme will be given first. The applicability of the calculation scheme will be demonstrated by comparing analytical, measured and simulated results.

[1]  Colin Campbell,et al.  Surface Acoustic Wave Devices for Mobile and Wireless Communications , 1998 .

[2]  D. Afolabi,et al.  Linearization of the quadratic eigenvalue problem , 1987 .

[3]  S. Joshi Flow sensor using surface acoustic waves , 1988, IEEE 1988 Ultrasonics Symposium Proceedings..

[4]  Yook-Kong Yong Analysis of periodic structures for BAW and SAW resonators , 2001, 2001 IEEE Ultrasonics Symposium. Proceedings. An International Symposium (Cat. No.01CH37263).

[5]  J. Z. Zhu,et al.  The finite element method , 1977 .

[6]  Anne-Christine Hladky-Hennion,et al.  Analysis of the propagation of plane acoustic waves in passive periodic materials using the finite element method , 1995 .

[7]  M. Handzic 5 , 1824, The Banality of Heidegger.

[8]  A. Majda,et al.  Radiation boundary conditions for acoustic and elastic wave calculations , 1979 .

[9]  B. Auld,et al.  Acoustic fields and waves in solids , 1973 .

[10]  Andrew Y. T. Leung,et al.  Inverse iteration for the quadratic eigenvalue problem , 1988 .

[11]  R. Weigel,et al.  Wireless pressure and temperature measurement using a SAW hybrid sensor , 2000, 2000 IEEE Ultrasonics Symposium. Proceedings. An International Symposium (Cat. No.00CH37121).

[12]  J.D.N. Cheeke,et al.  Surface acoustic wave humidity sensor based on the changes in the viscoelastic properties of a polymer film , 1996, 1996 IEEE Ultrasonics Symposium. Proceedings.

[13]  C. Rajakumar,et al.  Lanczos algorithm for the quadratic eigenvalue problem in engineering applications , 1993 .

[14]  A. Majda,et al.  Absorbing boundary conditions for the numerical simulation of waves , 1977 .

[15]  G. Kovacs,et al.  Improved Material Constants for LiNb03 and LiTaO3 , 1990 .

[16]  Leonhard Reindl,et al.  SAW devices as wireless passive sensors , 1996, 1996 IEEE Ultrasonics Symposium. Proceedings.

[17]  R. Bossut,et al.  Analysis of the scattering of a plane acoustic wave by a periodic elastic structure using the finite element method: Application to compliant tube gratings , 1990 .

[18]  F. Sandy,et al.  Reflection of Surfaces Waves from Periodic Discontinuities , 1976 .

[19]  K. Bathe Finite Element Procedures , 1995 .

[20]  R. Lerch,et al.  Simulation of piezoelectric devices by two- and three-dimensional finite elements , 1990, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[21]  Gregory C. Frye,et al.  Velocity and attenuation effects in acoustic wave chemical sensors , 1993 .

[22]  Robert L. Higdon,et al.  Radiation boundary conditions for elastic wave propagation , 1990 .

[23]  R. Weigel,et al.  SAW-based radio sensor systems , 2001, IEEE Sensors Journal.

[24]  U. Wolff,et al.  SAW sensors for harsh environments , 2001, IEEE Sensors Journal.

[25]  R. H. Tancrell,et al.  Acoustic surface wave filters , 1971 .

[26]  R. Dill,et al.  FEM analysis of the reflection coefficient of SAWs in an infinite periodic array , 1991, IEEE 1991 Ultrasonics Symposium,.

[27]  Donald C. Malocha,et al.  Remote sensor system using passive SAW sensors , 1994, 1994 Proceedings of IEEE Ultrasonics Symposium.

[28]  Peter Gudmundson,et al.  The usage of standard finite element codes for computation of dispersion relations in materials with periodic microstructure , 1997 .

[29]  J. Lysmer,et al.  Finite Dynamic Model for Infinite Media , 1969 .

[30]  J. Vartiainen,et al.  BAW radiation from LSAW resonators on lithium tantalate , 2001, 2001 IEEE Ultrasonics Symposium. Proceedings. An International Symposium (Cat. No.01CH37263).

[31]  B. Auld Acoustic fields and waves in solids. Vol. 1 , 1990 .

[32]  Jack Dongarra,et al.  Templates for the Solution of Algebraic Eigenvalue Problems , 2000, Software, environments, tools.

[33]  Maurice Petyt,et al.  A finite element study of harmonic wave propagation in periodic structures , 1974 .