{"title":"Lateral- and thickness-field coupling in lithium tetraborate","authors":"A. Ballato, J. Kosinski, M. Mizan, T. Lukaszek","doi":"10.1109/FREQ.1989.68917","DOIUrl":null,"url":null,"abstract":"Calculations have previously been made for rotated y-cuts, including the regions where the quasi-extensional and quasi-shear thickness modes have zero temperature coefficients of frequency. This work extends the calculations to doubly rotated bulk-wave resonators, and computes the coupling factors for the three simple-thickness modes driven by thickness (TE) and lateral (LE) quasistatic electric fields as a function of the orientation angles phi and theta , and the direction of the applied lateral field psi . Because of the temperature coefficients of the piezoelectric coupling factors, the temperature coefficient of a resonator depend not only upon orientation, but also upon harmonic number and location of the resonator operating point on the immittance circle. These considerations are addressed.<<ETX>>","PeriodicalId":294361,"journal":{"name":"Proceedings of the 43rd Annual Symposium on Frequency Control","volume":"4 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 43rd Annual Symposium on Frequency Control","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/FREQ.1989.68917","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 5
Abstract
Calculations have previously been made for rotated y-cuts, including the regions where the quasi-extensional and quasi-shear thickness modes have zero temperature coefficients of frequency. This work extends the calculations to doubly rotated bulk-wave resonators, and computes the coupling factors for the three simple-thickness modes driven by thickness (TE) and lateral (LE) quasistatic electric fields as a function of the orientation angles phi and theta , and the direction of the applied lateral field psi . Because of the temperature coefficients of the piezoelectric coupling factors, the temperature coefficient of a resonator depend not only upon orientation, but also upon harmonic number and location of the resonator operating point on the immittance circle. These considerations are addressed.<>