N. B. Chakrabarti, T. Rao, T. V. Rao, B. Roy, D. Bhattacharya
{"title":"用分层结构控制静磁波的色散","authors":"N. B. Chakrabarti, T. Rao, T. V. Rao, B. Roy, D. Bhattacharya","doi":"10.1109/ULTSYM.1987.198959","DOIUrl":null,"url":null,"abstract":"The dispersion relation of the magnetostatic surface wave propsgating in a ferrimagnetic double layer h as been found and the effects of v arious layers on the propagation characteristics have been examined. A linear delay variation extending from 125 ns/cm to 365 ns/cm over an 0.4 GHz bandwidth centered at 2.8 GHz is obtainable with YIG films of 10 micron thicknesses b ut with 4nM values as 1.75KG and 1.QKC respectfvely. havior of the magnetostatic surface wave propagation w ith in-plane magnetic field applied at an angle normal to the direction of propagation, has been studied and time delays have been computed as a function of this angle. Under this condition t he backward volume wzves are also generated along with surface waves\"he be","PeriodicalId":309261,"journal":{"name":"IEEE 1987 Ultrasonics Symposium","volume":"28 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dispersion Control of Magnetostatic Waves Using Layered Structure\",\"authors\":\"N. B. Chakrabarti, T. Rao, T. V. Rao, B. Roy, D. Bhattacharya\",\"doi\":\"10.1109/ULTSYM.1987.198959\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The dispersion relation of the magnetostatic surface wave propsgating in a ferrimagnetic double layer h as been found and the effects of v arious layers on the propagation characteristics have been examined. A linear delay variation extending from 125 ns/cm to 365 ns/cm over an 0.4 GHz bandwidth centered at 2.8 GHz is obtainable with YIG films of 10 micron thicknesses b ut with 4nM values as 1.75KG and 1.QKC respectfvely. havior of the magnetostatic surface wave propagation w ith in-plane magnetic field applied at an angle normal to the direction of propagation, has been studied and time delays have been computed as a function of this angle. Under this condition t he backward volume wzves are also generated along with surface waves\\\"he be\",\"PeriodicalId\":309261,\"journal\":{\"name\":\"IEEE 1987 Ultrasonics Symposium\",\"volume\":\"28 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE 1987 Ultrasonics Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ULTSYM.1987.198959\",\"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 1987 Ultrasonics Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ULTSYM.1987.198959","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Dispersion Control of Magnetostatic Waves Using Layered Structure
The dispersion relation of the magnetostatic surface wave propsgating in a ferrimagnetic double layer h as been found and the effects of v arious layers on the propagation characteristics have been examined. A linear delay variation extending from 125 ns/cm to 365 ns/cm over an 0.4 GHz bandwidth centered at 2.8 GHz is obtainable with YIG films of 10 micron thicknesses b ut with 4nM values as 1.75KG and 1.QKC respectfvely. havior of the magnetostatic surface wave propagation w ith in-plane magnetic field applied at an angle normal to the direction of propagation, has been studied and time delays have been computed as a function of this angle. Under this condition t he backward volume wzves are also generated along with surface waves"he be