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Surface Acoustic Waves in Z-Sections of Piezoelectric Monocrystals of Hexagonal Syngony

机译:六角合成的压电单晶体Z截面中的表面声波

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摘要

A new statement of the problem on the calculation of kinematic and dynamic characteristics of surface acoustic waves in piezoelectric monocrystals is proposed. A procedure for solving the above problem is also proposed with due regard for the existence of electric field scattering on the crystal surface not covered with electrodes and the vortex component of electric field in the general case.The procedure for mathematical description of surface acoustic waves at zero approximation is shown using an example of Z-section of monocrystals of hexagonal syngony. The system of eigenfunctions is built and eigenvalues are determined of the uniform boundary problem for the case of plain deformed state. The general solutions obtained for a particular case of isotropy of elastic properties of deformable solid body are reduced to the generally known definitions of the Rayleigh surface waves. The surface acoustic waves in Z-sections of ZnO and CdS monocrystals similar to the Rayleigh wave in isotropic elastic half-space are shown to exist in a narrow near-surface region, while taking into account the spread of electromagnetic field outside the limits of monocrystal on surfaces that are not covered with electrodes, and the vortex part of the electric field component made it possible to establish the fact that the vertical component of the shift vector of material particles had the maximum value at the depth of (0.15–0.2)λ rather than on the very surface of crystal. A similar peculiarity of Rayleigh waves is typical also for isotropic samples. The presence of local extremum (within 7%) is typical for the vertical component of shift vector in near-surface region having thickness 0.25λ. While penetrating inside the piezoelectric at the depth of more than 2.5 wavelength, the shift levels of material particles decrease by more than one order of magnitude.
机译:提出了一种关于压电单晶中表面声波的运动和动态特性计算的新陈述。还提出了解决上述问题的方法,以适当考虑到在未覆盖的晶体表面上的电场散射的存在,以及一般情况下的电场的涡流分量。表面声波的数学描述的过程使用六边形合成的单晶的Z-部分的示例显示零近似。构建特征函数的系统,并且确定了对普通变形状态的情况下的均匀边界问题的特征值。对于可变形固体弹性性质的各向同性的特定情况获得的一般溶液减少到瑞利表面波的通常已知的定义。 ZnO和Cds单晶中的表面声波类似于各向同性弹性半空间中的瑞利波的ZnO和Cds单晶的表面声波在狭窄的近表面区域中存在,同时考虑到电磁场在单晶体界限外的扩散在没有电极覆盖的表面上,电场部件的涡流部分使得可以确定材料颗粒的移位载体的垂直分量在(0.15-0.2)λ的深度处具有最大值。而不是在晶体的非常表面上。瑞利波的类似特殊性也是各向同性样品的典型。局部极值的存在(7%内)是典型的近表面区域的移位载体的垂直分量,其具有厚度为0.25λ。虽然在压电的深度处于超过2.5波长的深度渗透,但材料颗粒的换档水平减小了多种数量级。

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