A P-matrix based model for SAW grating waveguides taking into account modes conversion at the reflection

Several models exist for analyzing the wave-guiding effect of a reflective grating. On the one hand, there are models based on scalar waveguide theory. These models consider that a device can be described as being made of several regions having different velocities. On the other hand, an extension of the coupling of modes (COM) model taking into account the transverse dimension has been developed. This paraxial COM model predicts that guidance is possible even when there is no velocity difference between the interior and the exterior of the grating region. Guidance, under such circumstances, is due only to differences in reflectivity between regions. Following from this insight, a new approach has been developed: guided modes and the continuum of radiating modes are first determined. At each period, reflections then are considered as occurring only in the reflective regions, so that the modes are truncated. Thus, at each reflection (and transmission), each mode is converted into a distribution of all modes. Dispersion curves very similar to those shown by other researchers are obtained by this method. They show, in particular, the existence of guided modes even when the wave velocity in all regions is identical. This model can be used to more easily analyze practical devices and exhibits a good agreement with experimental results.

[1]  L. Coldren,et al.  Thin Fiim Acoustic Surface Waveguides on Anisotropic Media , 1975, IEEE Transactions on Sonics and Ultrasonics.

[2]  P. Ventura,et al.  Combined FEM and Green's function analysis of periodic SAW structure, application to the calculation of reflection and scattering parameters , 2001, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[3]  Mode profiles in waveguide-coupled resonators , 1992, IEEE 1992 Ultrasonics Symposium Proceedings.

[4]  G. Farnell,et al.  Diffraction and Beam Steering for Surface-Wave Comb Structures on Anisotropic Substrates , 1971, IEEE Transactions on Sonics and Ultrasonics.

[5]  M. Solal A P-matrix-based model for the analysis of SAW transversely coupled resonator filters, including guided modes and a continuum of radiated waves , 2003, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[7]  K. Hashimoto,et al.  Analysis of Surface Acoustic Waves Obliquely Propagating under Metallic Gratings with Finite Thickness , 1996 .

[8]  V. Laude,et al.  Slowness curves and characteristics of surface acoustic waves propagating obliquely in periodic finite-thickness electrode gratings , 2003 .

[9]  S. Jen,et al.  112/spl deg/-LiTaO/sub 3/ periodic waveguides , 1995, 1995 IEEE Ultrasonics Symposium. Proceedings. An International Symposium.

[10]  K. Hirota,et al.  Analysis of SAW grating waveguides using 2-D coupling-of-modes equations , 2001, 2001 IEEE Ultrasonics Symposium. Proceedings. An International Symposium (Cat. No.01CH37263).

[11]  M. Mayer,et al.  A powerful novel method for the simulation of waveguiding in SAW devices , 2003, IEEE Symposium on Ultrasonics, 2003.

[12]  Peter Russer,et al.  P-matrix modeling of transverse-mode coupled resonator filters , 1993 .

[13]  Marc Solal,et al.  Numerical methods for SAW propagation characterization , 1998, 1998 IEEE Ultrasonics Symposium. Proceedings (Cat. No. 98CH36102).

[14]  M. Solal,et al.  A new triply rotated quartz cut for the fabrication of low loss IF SAW filters , 2004, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[15]  M. Solal,et al.  A new triply rotated quartz cut for the fabrication of low loss SAW filters , 2000, 2000 IEEE Ultrasonics Symposium. Proceedings. An International Symposium (Cat. No.00CH37121).

[16]  Hermann A. Haus,et al.  Modes in SAW grating resonators , 1977 .