{"title":"非线性参数B/A的超声反射模式成像:理论基础","authors":"C. Cain","doi":"10.1109/ULTSYM.1985.198640","DOIUrl":null,"url":null,"abstract":"The theoretical basis of a new method for obtaining reflection mode images of the nonlinear parameter B/A is given. An expression for the instantaneous phase shift in a reflected sinusoidal probe due to nonlinear interaction with an arbitrary pump waveform propagating in the opposite direction is derived. This i nstantaneous phase shift is proportional to the convolution of the pump waveform with the spatial d istribution of the nonlinear parameter B/A along the propagation path of the pump and interacting probe. If a linear frequency modulated (LFM) sinusoid is used for t he probe, then the pump interacts with the reflected probe at each point in space at a unique frequency . This u seful property simplifies signal processing and leads to algorithms for separation of the desired from undesired reflections in a r ever be rant env i r onmen t .","PeriodicalId":240321,"journal":{"name":"IEEE 1985 Ultrasonics Symposium","volume":"44 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":"{\"title\":\"Ultrasonic Reflection Mode Imaging of the Nonlinear Parameter B/A: A Theoretical Basis\",\"authors\":\"C. Cain\",\"doi\":\"10.1109/ULTSYM.1985.198640\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The theoretical basis of a new method for obtaining reflection mode images of the nonlinear parameter B/A is given. An expression for the instantaneous phase shift in a reflected sinusoidal probe due to nonlinear interaction with an arbitrary pump waveform propagating in the opposite direction is derived. This i nstantaneous phase shift is proportional to the convolution of the pump waveform with the spatial d istribution of the nonlinear parameter B/A along the propagation path of the pump and interacting probe. If a linear frequency modulated (LFM) sinusoid is used for t he probe, then the pump interacts with the reflected probe at each point in space at a unique frequency . This u seful property simplifies signal processing and leads to algorithms for separation of the desired from undesired reflections in a r ever be rant env i r onmen t .\",\"PeriodicalId\":240321,\"journal\":{\"name\":\"IEEE 1985 Ultrasonics Symposium\",\"volume\":\"44 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"10\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE 1985 Ultrasonics Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ULTSYM.1985.198640\",\"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 1985 Ultrasonics Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ULTSYM.1985.198640","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Ultrasonic Reflection Mode Imaging of the Nonlinear Parameter B/A: A Theoretical Basis
The theoretical basis of a new method for obtaining reflection mode images of the nonlinear parameter B/A is given. An expression for the instantaneous phase shift in a reflected sinusoidal probe due to nonlinear interaction with an arbitrary pump waveform propagating in the opposite direction is derived. This i nstantaneous phase shift is proportional to the convolution of the pump waveform with the spatial d istribution of the nonlinear parameter B/A along the propagation path of the pump and interacting probe. If a linear frequency modulated (LFM) sinusoid is used for t he probe, then the pump interacts with the reflected probe at each point in space at a unique frequency . This u seful property simplifies signal processing and leads to algorithms for separation of the desired from undesired reflections in a r ever be rant env i r onmen t .