{"title":"Impact of In-Plane Diffraction in Temperature Compensated Surface Acoustic Wave Resonator on SiO2/131°YX-LiNbO3 Structure","authors":"Yiming Liu;Yiwen He;Ting Wu;Zijiang Yang;Fangyi Li;Jingfu Bao;Ken-Ya Hashimoto","doi":"10.1109/TUFFC.2025.3566466","DOIUrl":null,"url":null,"abstract":"This article investigates impact of in-plane surface acoustic wave (SAW) diffraction on the Bode Q curve in temperature compensated (TC) SAW resonators on 131°YX-LiNbO3 (131-LN). The right figure compares measured TC-SAW resonator characteristics with theoretical ones obtained by the periodic and full 3-D finite element method (FEM). Estimated ohmic resistance is subtracted from the measured result. The result of full 3-D FEM agrees very well with the experiment even Bode Q although no additional loss is included in the simulation. Full 3-D FEM can explain Bode Q variation with the number of IDT finger pairs (<inline-formula> <tex-math>${N} _{\\text {I}}$ </tex-math></inline-formula>) and aperture length (W) well. This means that the in-plane SAW diffraction is one of the major loss mechanisms in TC-SAW devices. Next, the piston mode design is applied to the TC-SAW structure for the removal of transverse mode resonances, and the full 3-D FEM simulation is applied for wide range of W and <inline-formula> <tex-math>${N} _{\\text {I}}$ </tex-math></inline-formula>. It is shown that the TC-SAW resonators suffer significant Bode Q degradation by the in-plane SAW diffraction, and its impact is more severe than the incredible high-performance (I.H.P.) SAW case. Namely, the Bode Q of TC-SAW resonators is more sensitive to f, W, and <inline-formula> <tex-math>${N} _{\\text {I}}$ </tex-math></inline-formula> than that of I.H.P. SAW resonators due to the convex SAW slowness shape on the surface.","PeriodicalId":13322,"journal":{"name":"IEEE transactions on ultrasonics, ferroelectrics, and frequency control","volume":"72 7","pages":"996-1003"},"PeriodicalIF":3.7000,"publicationDate":"2025-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE transactions on ultrasonics, ferroelectrics, and frequency control","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10982348/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ACOUSTICS","Score":null,"Total":0}
引用次数: 0
Abstract
This article investigates impact of in-plane surface acoustic wave (SAW) diffraction on the Bode Q curve in temperature compensated (TC) SAW resonators on 131°YX-LiNbO3 (131-LN). The right figure compares measured TC-SAW resonator characteristics with theoretical ones obtained by the periodic and full 3-D finite element method (FEM). Estimated ohmic resistance is subtracted from the measured result. The result of full 3-D FEM agrees very well with the experiment even Bode Q although no additional loss is included in the simulation. Full 3-D FEM can explain Bode Q variation with the number of IDT finger pairs (${N} _{\text {I}}$ ) and aperture length (W) well. This means that the in-plane SAW diffraction is one of the major loss mechanisms in TC-SAW devices. Next, the piston mode design is applied to the TC-SAW structure for the removal of transverse mode resonances, and the full 3-D FEM simulation is applied for wide range of W and ${N} _{\text {I}}$ . It is shown that the TC-SAW resonators suffer significant Bode Q degradation by the in-plane SAW diffraction, and its impact is more severe than the incredible high-performance (I.H.P.) SAW case. Namely, the Bode Q of TC-SAW resonators is more sensitive to f, W, and ${N} _{\text {I}}$ than that of I.H.P. SAW resonators due to the convex SAW slowness shape on the surface.
期刊介绍:
IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control includes the theory, technology, materials, and applications relating to: (1) the generation, transmission, and detection of ultrasonic waves and related phenomena; (2) medical ultrasound, including hyperthermia, bioeffects, tissue characterization and imaging; (3) ferroelectric, piezoelectric, and piezomagnetic materials, including crystals, polycrystalline solids, films, polymers, and composites; (4) frequency control, timing and time distribution, including crystal oscillators and other means of classical frequency control, and atomic, molecular and laser frequency control standards. Areas of interest range from fundamental studies to the design and/or applications of devices and systems.