{"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}
引用次数: 10
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 .