Temperature Dependence of Surface Acoustic Wave Propagation Velocity in InxGa1-xN Films Obtained by High-Resolution Brillouin Spectroscopy: Determination of Temperature Coefficient of Frequency

2013 ◽  
Vol 6 (5) ◽  
pp. 056601 ◽  
Author(s):  
Rafael J. Jiménez Riobóo ◽  
Carlos Prieto ◽  
Ramón Cuscó ◽  
Lluís Artús ◽  
Chris Boney ◽  
...  
2011 ◽  
Vol 56 (5) ◽  
pp. 632-636 ◽  
Author(s):  
D. S. Sanditov ◽  
A. A. Mashanov ◽  
B. D. Sanditov ◽  
S. Sh. Sangadiev

1999 ◽  
Vol 11 (5) ◽  
pp. 1065-1080 ◽  
Author(s):  
Peter D. M. Spelt ◽  
Michael A. Norato ◽  
Ashok S. Sangani ◽  
Lawrence L. Tavlarides

2018 ◽  
Vol 2018 ◽  
pp. 1-7 ◽  
Author(s):  
Yuxia Yang ◽  
Koji Nagano ◽  
Tatsuo Iwasa ◽  
Hisashi Fukuda

We describe the measurement of surface acoustic wave (SAW) velocities to identify five odorant molecules by using a SAW device system. We derive a new frequency equation for SAWs propagating in the SAW device system with Cynops pyrrhogaster lipocalin (Cp-Lip1) protein, in order to identify five odorant molecules, R-limonene (R-Lim), ethyl butyrate (Eth), 2-isobutylthiazole (Iso), benzophenone (Ben), and 2-acetylthiazole (Ace). We developed a method to identify these odorant molecules combined with the Cp-Lip1 odorant-binding protein. Our frequency equation can satisfactorily predict different odorant molecules in the Cp-Lip1 SAW device. Moreover, our data suggest that the propagation velocity of the SAWs mostly relate to the density and concentration of the Cp-Lip1 odorant molecule mixtures. At the same sample concentration, the propagation velocity depends on the density. For the same odorant molecule, the propagation velocity decreases with increasing concentration.


2011 ◽  
Vol 267 ◽  
pp. 561-564
Author(s):  
Zhong Ning Zhang ◽  
Jian Tian

For the problem of acoustic emission source location, it has always been one of the important issues to look for simple and convenient layout of sensors. This paper presents a new time difference method for locating acoustic emission source in a plate, which the sensors for locating are arranged in a straight line, and does not need the pre-determining of the acoustic wave propagation velocity. The method makes the acoustic emission source locating task simplified.


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