{"title":"静电可变锯片延迟线。理论和实验","authors":"A. Budreau, G. Scalzi, P. Carr, H. Bertoni","doi":"10.1109/T-SU.1984.31550","DOIUrl":null,"url":null,"abstract":"A theoretical and experimental investigation has been made of surface acoustic wave (SAW) timedelay change produced by the application of a dc electric field. Measurements were made on the three high-coupling cuts of lithium niobate for the electric field applied in the plane of the surface with a novel electrode configuration and normal-tothe- surface with a standard \"convolver\" plate. A theory has been developed for the normal field configuration, where the electric field is uniform, and for the in-plane case, where the field is nonuniform. The dominant contribution for the latterc omes from the center of the electrodes. For the 38 X-cut of lithium niobate, the normal field sensitivity (fractional timedelay change per applied electric field γ). is 141x10-12m/V, while γ for the in-plane field is 6x10-12m/V. The in-plane configuration has the advantage of having lower insertion loss and dispersion as the SAW does not have to propagate through a metal electrode. For 16.5° doubly rotated lithium niobate, a normal field device with a substrate thickness of 0.16 mm yielded a fractional timedelay change of 0.9x10-6/V. To our knowledge this is the largest time-delay change per applied voltage yet reported. The time-delay change is 10-4very linear with applied voltage; the second derivative is typically multiplied by slope. Both electrode configurations yield monolithic devices that dissipate no dc power.","PeriodicalId":371797,"journal":{"name":"IEEE Transactions on Sonics and Ultrasonics","volume":"74 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1984-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Electrostatically variable saw delay lines - Theory and experiment\",\"authors\":\"A. Budreau, G. Scalzi, P. Carr, H. Bertoni\",\"doi\":\"10.1109/T-SU.1984.31550\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A theoretical and experimental investigation has been made of surface acoustic wave (SAW) timedelay change produced by the application of a dc electric field. Measurements were made on the three high-coupling cuts of lithium niobate for the electric field applied in the plane of the surface with a novel electrode configuration and normal-tothe- surface with a standard \\\"convolver\\\" plate. A theory has been developed for the normal field configuration, where the electric field is uniform, and for the in-plane case, where the field is nonuniform. The dominant contribution for the latterc omes from the center of the electrodes. For the 38 X-cut of lithium niobate, the normal field sensitivity (fractional timedelay change per applied electric field γ). is 141x10-12m/V, while γ for the in-plane field is 6x10-12m/V. The in-plane configuration has the advantage of having lower insertion loss and dispersion as the SAW does not have to propagate through a metal electrode. For 16.5° doubly rotated lithium niobate, a normal field device with a substrate thickness of 0.16 mm yielded a fractional timedelay change of 0.9x10-6/V. To our knowledge this is the largest time-delay change per applied voltage yet reported. The time-delay change is 10-4very linear with applied voltage; the second derivative is typically multiplied by slope. Both electrode configurations yield monolithic devices that dissipate no dc power.\",\"PeriodicalId\":371797,\"journal\":{\"name\":\"IEEE Transactions on Sonics and Ultrasonics\",\"volume\":\"74 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1984-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Transactions on Sonics and Ultrasonics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/T-SU.1984.31550\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Transactions on Sonics and Ultrasonics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/T-SU.1984.31550","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electrostatically variable saw delay lines - Theory and experiment
A theoretical and experimental investigation has been made of surface acoustic wave (SAW) timedelay change produced by the application of a dc electric field. Measurements were made on the three high-coupling cuts of lithium niobate for the electric field applied in the plane of the surface with a novel electrode configuration and normal-tothe- surface with a standard "convolver" plate. A theory has been developed for the normal field configuration, where the electric field is uniform, and for the in-plane case, where the field is nonuniform. The dominant contribution for the latterc omes from the center of the electrodes. For the 38 X-cut of lithium niobate, the normal field sensitivity (fractional timedelay change per applied electric field γ). is 141x10-12m/V, while γ for the in-plane field is 6x10-12m/V. The in-plane configuration has the advantage of having lower insertion loss and dispersion as the SAW does not have to propagate through a metal electrode. For 16.5° doubly rotated lithium niobate, a normal field device with a substrate thickness of 0.16 mm yielded a fractional timedelay change of 0.9x10-6/V. To our knowledge this is the largest time-delay change per applied voltage yet reported. The time-delay change is 10-4very linear with applied voltage; the second derivative is typically multiplied by slope. Both electrode configurations yield monolithic devices that dissipate no dc power.