2014
DOI: 10.1016/j.physe.2014.02.001
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Tunable passband in one-dimensional phononic crystal containing a piezoelectric 0.62Pb(Mg1/3Nb2/3)O3–0.38PbTiO3 single crystal defect layer

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Cited by 39 publications
(25 citation statements)
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“…As a defect, a 0.2mol% Fe-doped relaxor-based ferroelectric 0.62PB(MG 1/3 NB 1/3 )O 3 -0.38PBTIO 3 (PNM-0.38PT) layer was introduced into the structures. The use of this material allows to control, to a certain extent, the location of the transmission peaks as shown by (Wang et al (2014)). In the analyzed range of ultrasonic wave frequencies, there were from three to six transmission peaks for all types of structures.…”
Section: Discussionmentioning
confidence: 99%
“…As a defect, a 0.2mol% Fe-doped relaxor-based ferroelectric 0.62PB(MG 1/3 NB 1/3 )O 3 -0.38PBTIO 3 (PNM-0.38PT) layer was introduced into the structures. The use of this material allows to control, to a certain extent, the location of the transmission peaks as shown by (Wang et al (2014)). In the analyzed range of ultrasonic wave frequencies, there were from three to six transmission peaks for all types of structures.…”
Section: Discussionmentioning
confidence: 99%
“…Besides the above-mentioned three introduced materials, another smart material, which is the fourth introduced material, is the piezoelectric material, which is also dependent on electric fields like the dielectric elastomer, which has been extensively used in periodically laminated structures, i.e., one-dimensional (1D) piezoelectric layered phononic crystals. Because the electrical field is relatively easy to control and the piezoelectric effect is linear coupling between the electrical and mechanical fields, the elastic wave propagation and its tuning by the electrical conditions in periodically laminated piezoelectric composites have received extensive attention during the last two decades [29][30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48]. The earlier literatures on this topic only considered the relatively simple electrical boundaries, i.e., the electric-open and electric-short conditions.…”
Section: Introductionmentioning
confidence: 99%
“…More specifically, modifying the contrast in material parameters of a crystal, or changing the physical arrangement of components, manifests in the transmission spectrum and band structure to show the effects on transient sound. Active sonic structures with applied static electric fields, [14][15][16] magnetically, [17][18][19] mechanically 20,21 and recently with infrared radiation 22 have been reported. Most of these active sonic structures are in physical contact with the actuating source.…”
Section: Introductionmentioning
confidence: 99%