{"title":"k²₃₃Estimation of Thin Films via Piezoelectric Stiffening Using Ultrasonic Reflectometry","authors":"Yohkoh Shimano;Motoshi Suzuki;Takahiko Yanagitani","doi":"10.1109/OJUFFC.2025.3537962","DOIUrl":null,"url":null,"abstract":"A method for estimating intrinsic electromechanical coupling coefficient <inline-formula> <tex-math>${k}_{{33}}^{{2}}$ </tex-math></inline-formula> of piezoelectric thin films using piezoelectrically stiffened acoustic velocity <inline-formula> <tex-math>${V}^{\\text {D}}$ </tex-math></inline-formula> and unstiffened acoustic velocity <inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula> was proposed. <inline-formula> <tex-math>${V}^{\\text {D}}$ </tex-math></inline-formula> and <inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula> velocities of thin films in the sub-GHz range were estimated by ultrasonic reflectometry. Directly depositing a film specimen on the backside of the ultrasonic delay line eliminates the need for a coupler layer and avoids acoustic attenuation in the layer. The <inline-formula> <tex-math>${V}^{\\text {D}}$ </tex-math></inline-formula> velocity can be estimated from the phase differences of the echoes: before and after the film specimen is deposited. In contrast, <inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula> velocity can be estimated from the phase difference when the film specimen is under the open circuit and the short circuit. The intrinsic <inline-formula> <tex-math>${k}_{{33}}^{{2}}{}$ </tex-math></inline-formula> can be obtained from the relationship of <inline-formula> <tex-math>${k}_{{33}}^{{2}}~\\text {=}$ </tex-math></inline-formula> 1 – (<inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula>/<inline-formula> <tex-math>${V}^{\\text {D}})^{{2}}$ </tex-math></inline-formula>. For the Sc0.4Al0.6N thin film specimen, <inline-formula> <tex-math>${k}_{{33}}^{{2}}$ </tex-math></inline-formula> was determined to be 11.6% from <inline-formula> <tex-math>${V}^{\\text {D}}$ </tex-math></inline-formula> and <inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula> of 8400 m/s and 7900 m/s, respectively. For the ZnO thin film specimen, <inline-formula> <tex-math>${k}_{{33}}^{{2}}$ </tex-math></inline-formula> was estimated to be 4.7% from <inline-formula> <tex-math>${V}^{\\text {D}}$ </tex-math></inline-formula> and <inline-formula> <tex-math>${V}^{\\text {E}}$ </tex-math></inline-formula> of 6250 m/s and 6100 m/s, respectively. These values are in good agreement with previously reported results.","PeriodicalId":73301,"journal":{"name":"IEEE open journal of ultrasonics, ferroelectrics, and frequency control","volume":"5 ","pages":"6-10"},"PeriodicalIF":0.0000,"publicationDate":"2025-02-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=10869444","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE open journal of ultrasonics, ferroelectrics, and frequency control","FirstCategoryId":"1085","ListUrlMain":"https://ieeexplore.ieee.org/document/10869444/","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
A method for estimating intrinsic electromechanical coupling coefficient ${k}_{{33}}^{{2}}$ of piezoelectric thin films using piezoelectrically stiffened acoustic velocity ${V}^{\text {D}}$ and unstiffened acoustic velocity ${V}^{\text {E}}$ was proposed. ${V}^{\text {D}}$ and ${V}^{\text {E}}$ velocities of thin films in the sub-GHz range were estimated by ultrasonic reflectometry. Directly depositing a film specimen on the backside of the ultrasonic delay line eliminates the need for a coupler layer and avoids acoustic attenuation in the layer. The ${V}^{\text {D}}$ velocity can be estimated from the phase differences of the echoes: before and after the film specimen is deposited. In contrast, ${V}^{\text {E}}$ velocity can be estimated from the phase difference when the film specimen is under the open circuit and the short circuit. The intrinsic ${k}_{{33}}^{{2}}{}$ can be obtained from the relationship of ${k}_{{33}}^{{2}}~\text {=}$ 1 – (${V}^{\text {E}}$ /${V}^{\text {D}})^{{2}}$ . For the Sc0.4Al0.6N thin film specimen, ${k}_{{33}}^{{2}}$ was determined to be 11.6% from ${V}^{\text {D}}$ and ${V}^{\text {E}}$ of 8400 m/s and 7900 m/s, respectively. For the ZnO thin film specimen, ${k}_{{33}}^{{2}}$ was estimated to be 4.7% from ${V}^{\text {D}}$ and ${V}^{\text {E}}$ of 6250 m/s and 6100 m/s, respectively. These values are in good agreement with previously reported results.