Background, Motivation and Objective With the ultrafast development of information technology, there are urgent demands for acoustic wave devices that can be working at high and/or multiple frequency ranges, because t...
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ISBN:
(纸本)9781509011902
Background, Motivation and Objective With the ultrafast development of information technology, there are urgent demands for acoustic wave devices that can be working at high and/or multiple frequency ranges, because these acoustic wave devices are the core components of intelligent devices with rapid-responsibility and multi-functionality. These acoustic wave devices may be realized through the advanced rod-type piezoelectric phononic crystals, which consist of periodically-arranged piezoelectric rod covered by electrodes and elastic rod. Because the longitudinal wave is relatively easy to manipulate even at high frequency ranges and the longitudinal waves in rod-type piezoelectric phononic crystals possess tunable band structures. Consequently, the analysis of longitudinal wave bands in rod-type piezoelectric phononic crystals, particularly the effect of various applied electrical boundary conditions on the band structures, is significant for the design of these wave devices. So far, analytical-based methods such as the transfer matrix method(TMM), the combination of spectral element method(SEM) and TMM, the Analytical Method(AM), and numerical-based methods such as the finite element method(FEM) have been proposed for the analysis of longitudinal wave bands in rod-type piezoelectric phononic crystals. Unfortunately, the analytical-based methods cease to be effective in the high frequency range since the classical rod theory was adopted, which is only valid within pretty low frequency range. The numerical-based method may be inefficient for the high frequency analysis since large number of elements and very small time step are required in this case. In order to analyze the high-frequency longitudinal wave bands in rod-type piezoelectric phononic crystals, a modified transfer matrix method(MTMM) is presented, which adopts the method of reverberation-ray matrix(MRRM) to derive the local transfer matrices of structural members. The tunability of longitudinal-wave band
Ba0.6Sr0.4TiO3/Mg1-xZnxO(MZO,x=0,0.05,0.10,0.15 and 0.20) ceramic composites were prepared by traditional ceramic *** crystal structure,fracture surface morphology,and dielectric properties were *** samples with x=0,0...
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Ba0.6Sr0.4TiO3/Mg1-xZnxO(MZO,x=0,0.05,0.10,0.15 and 0.20) ceramic composites were prepared by traditional ceramic *** crystal structure,fracture surface morphology,and dielectric properties were *** samples with x=0,0.05 and 0.10 exhibited favorable sintering behavior,and homogeneous diphase microstructure was obtained. Nevertheless,the microstructure of the samples with x=0.15 and 0.20 was inhomogeneous and abnormal grain growth could be observed,and the abnormal grain growth induced the degradation of dielectric *** sample with x=0.10 has relatively low dielectric loss(1.26×10-3) and the optimal FOM value(about 174) .
BaTi4O9-doped Ba0.6Sr0.4TiO3(BST) composite ceramics were prepared by the conventional solid-state reaction and their structure,dielectric nonlinear characteristics and microwave dielectric properties were *** seconda...
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BaTi4O9-doped Ba0.6Sr0.4TiO3(BST) composite ceramics were prepared by the conventional solid-state reaction and their structure,dielectric nonlinear characteristics and microwave dielectric properties were *** secondary phase of the orthorhombic structure Ba4Ti13O30 is formed among BST composite ceramics with the increase of *** the same time,a duplex or bimodal grains size distribution shows fine grains in a coarse grain *** degree of frequency dispersion of dielectric permittivity below Tm is increased initially and then decreased with respect to *** the BaTi4O9 content increases,the tunability of composite ceramics decreases,while the Q value ***,70 wt%BaTi4O9-doped BST has a tunability~4.0%(under 30 kV/cm biasing) versus a permittivity~68 and quality factor ~134.1(at~3.2 GHz) .
The electron-phonon coupling (EPC) in solids is the fundamental coupling related with their phonons and electronic *** the conventional EPC research,the phonons and electrons are in the same dimension regime,generally...
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The electron-phonon coupling (EPC) in solids is the fundamental coupling related with their phonons and electronic *** the conventional EPC research,the phonons and electrons are in the same dimension regime,generally in the three-dimensional (3D) regime,which limits the tunability of EPC in solids.
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