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首页> 外文期刊>Journal of Experimental and Theoretical Physics >Phase resonance in the reflection of acoustic waves by a system of piezocrystalline layers separated by cladding layers with screening properties
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Phase resonance in the reflection of acoustic waves by a system of piezocrystalline layers separated by cladding layers with screening properties

机译:压电晶体系统的声波反射中的相位共振,该压电晶体系统由具有屏蔽特性的包层隔开

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We discuss the reflection of a transverse elastic wave incident from a substrate onto a system consisting of a periodic system of piezocrystalline layers with identical material properties, one side of which is bounded by the substrate and the other by a mechanically free surface. The layers are separated by superconducting or metallized cladding layers, depending on whether the layers are made of piezomagnetic or piezoelectric material, respectively. Because these cladding layers screen the quasistatic magnetic or electric fields that accompany the elastic wave, they cause a reflection of the wave at the layer boundaries that is weak due to the smallness of the magneto- or electromechanical coupling parameters. The presence of the mechanically free surface ensures total reflection at any angle of incidence, so that the amplitude of the reflection coefficient is always unity. This allows us to study the effects of diffraction on the phase of the reflection coefficient for a wave reflected from the boundary of the substrate-layered structure against this constant (unity) amplitude background. We have analyzed the spectral dependence of the phase change of the reflected wave due to multiple reflection at the boundaries between layers, which adds to the path length of the wave. We show that this diffraction-induced phase shift has a characteristic resonance behavior, attaining a maximum value near Bragg-forbidden zones that is roughly twice the increase in the maximum background level. We discuss several possible wave effects based on the concept of phase resonance.
机译:我们讨论了从基底入射到由具有相同材料特性的压电层的周期性系统组成的系统组成的系统的横向弹性波的反射,该系统的一侧受基底限制,而另一侧受机械自由表面限制。取决于层是分别由压电材料还是压电材料制成,这些层被超导或金属化的包层分开。因为这些包层屏蔽了弹性波所伴随的准静态磁场或电场,所以它们会由于电磁耦合参数较小而在层边界处反射弱的反射波。机械自由表面的存在确保了在任何入射角下的全反射,因此反射系数的振幅始终是统一的。这使我们能够研究在恒定(统一)振幅背景下从衬底层结构的边界反射的波的衍射对反射系数相位的影响。我们已经分析了由于在层之间的边界处多次反射而导致的反射波相位变化的频谱依赖性,这增加了波的路径长度。我们表明,这种由衍射引起的相移具有特征性的共振行为,在布拉格禁区附近获得的最大值大约是最大背景水平增加的两倍。我们将基于相位共振的概念讨论几种可能的波效应。

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