Mapping the band structure of a surface phononic crystal

We map the band structure of surface acoustic modes of a periodic array of copper lines embedded in a SiO2 film on a silicon substrate by means of the laser-induced transient grating technique. A detailed map of the lowest sheet of the ω(k) surface and partial maps of two higher-order sheets are obt...

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Bibliographic Details
Main Authors: Maznev, Alexei (Contributor), Wright, O. B. (Author), Matsuda, Osamu (Author)
Other Authors: Massachusetts Institute of Technology. Department of Chemistry (Contributor)
Format: Article
Language:English
Published: Institute of Physics Publishing, 2012-05-04T14:55:17Z.
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Online Access:Get fulltext
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100 1 0 |a Maznev, Alexei  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Chemistry  |e contributor 
100 1 0 |a Maznev, Alexei  |e contributor 
100 1 0 |a Maznev, Alexei  |e contributor 
700 1 0 |a Wright, O. B.  |e author 
700 1 0 |a Matsuda, Osamu  |e author 
245 0 0 |a Mapping the band structure of a surface phononic crystal 
260 |b Institute of Physics Publishing,   |c 2012-05-04T14:55:17Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/70497 
520 |a We map the band structure of surface acoustic modes of a periodic array of copper lines embedded in a SiO2 film on a silicon substrate by means of the laser-induced transient grating technique. A detailed map of the lowest sheet of the ω(k) surface and partial maps of two higher-order sheets are obtained. We discuss the topology of the ω(k) surface and explain how it arises from the Rayleigh and Sezawa modes of the film/substrate system. In the vicinity of the bandgap formed at the Brillouin zone boundary, the first and second dispersion sheets take the form of a saddle and a bowl, respectively, in agreement with a weak perturbation model. The shape of the third dispersion sheet, however, appears to defy expectations based on the perturbation approach. In particular, it contains minima located off the symmetry directions, which implies the existence of zero group velocity modes with an obliquely directed wavevector. 
520 |a United States. Dept. of Energy (Office of Science, and Office of Basic Energy Sciences, S3TEC Energy Frontier Research Center under award no. DE-SC0001088) 
546 |a en_US 
655 7 |a Article 
773 |t New Journal of Physics