Abstract
In this paper the theory of the elastic wave resonance reflection from a thin solid layer inserted into a crystal is developed for the angles of incidence corresponding to the excitation of the leaky wave, which arises from the bulk wave propagating in the crystal with group velocity parallel to the layer. It is shown that within some narrow interval of angles of incidence the coefficients of transformation undergo strong and abrupt changes in their magnitudes and phases. For example, it may occur that under resonance conditions the incident wave will reflect almost totally from the layer, whereas outside the resonance region of angles of incidence it transmits almost totally through the layer.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
