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Imaging Acoustic Waves by Microwave Microscopy: Microwave Impedance Microscopy for Visualizing Gigahertz Acoustic Waves

机译:通过微波显微镜进行成像声波:微波阻抗显微镜可视化千兆赫兹声波

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摘要

Atoms in all materials are constantly shaking, which is largely responsible for the transfer of heat and sound. In a uniform crystalline solid, the motion of the lattice can be decomposed into just a handful of normal modes of vibration or, in the language of quantum mechanics, a set of quantized eigenmodes of the elastic structure known as phonons [1]. In the frequency (f) regime of interest for microwave engineers, there exist three (one longitudinal, two shear) branches of vibrational modes with long wavelengths-"long" when compared with the atomic spacing. Their frequencies, which represent the energy of each quantum, are linearly proportional to the inverse wavelengths, which represent the momentum of each quantum. The ratio between the two is typically several kilometers per second. In good crystals with few imperfections, these vibrations travel a very long distance-"long" when compared with the wavelength-with little decay of the amplitude under the ambient temperature and pressure. At audio frequencies, these sound waves can propagate in solids. They are commonly known as acoustic waves (see "Nomenclature Used Throughout").
机译:所有材料中的原子不断摇动,这主要负责传递热量和声音。在均匀的结晶固体中,晶格的运动可以只是少数正常的振动模式,或者在量子力学的语言中,这是一种称为声子的弹性结构的量化特征模度[1]。在微波工程师的频率(f)的景点中,与原子间距相比,存在具有长波长的振动模式的三个(一个纵向,两个剪切)分支,与原子间距相比。它们代表每个量子的能量的频率与反波长线性成比例,其代表每个量子的动量。两者之间的比例通常为每秒几公里。在缺乏缺陷的晶体中,与波长 - 在环境温度和压力下的波长衰减时,这些振动在与幅度的衰减很小的衰减时,这些振动行进了很长的距离 - “长”。在音频频率下,这些声波可以以固体传播。它们通常称为声波(参见始终使用的“命名法”)。

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