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Journal articles on the topic 'Surface acoustics wave'

Author: Grafiati

Published: 8 June 2024

Last updated: 31 July 2025

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1

Daigle, G. A., and T. F. W. Embleton. "Surface waves and surface wave devices in atmospheric acoustics." Journal of the Acoustical Society of America 88, S1 (1990): S190. http://dx.doi.org/10.1121/1.2028857.

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2

Nakano, Masahiro. "Surface acoustic wave element, surface acoustic wave device, surface acoustic wave duplexer, and method of manufacturing surface acoustic wave element." Journal of the Acoustical Society of America 121, no. 4 (2007): 1826. http://dx.doi.org/10.1121/1.2723967.

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3

Krylov, Victor V. "On the Applicability of Kramers–Kronig Dispersion Relations to Guided and Surface Waves." Acoustics 6, no. 3 (2024): 610–19. http://dx.doi.org/10.3390/acoustics6030033.

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In unbounded media, the acoustic attenuation as function of frequency is related to the frequency-dependent sound velocity (dispersion) via Kramers–Kronig dispersion relations. These relations are fundamentally important for better understanding of the nature of attenuation and dispersion and as a tool in physical acoustics measurements, where they can be used for control purposes. However, physical acoustic measurements are frequently carried out not in unbounded media but in acoustic waveguides, e.g., inside liquid-filled pipes. Surface acoustic waves are also often used for physical acousti

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4

Gokani, Chirag A., Thomas S. Jerome, Michael R. Haberman, and Mark F. Hamilton. "Born approximation of acoustic radiation force used for acoustofluidic separation." Journal of the Acoustical Society of America 151, no. 4 (2022): A90. http://dx.doi.org/10.1121/10.0010753.

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Acoustofluidic separation often involves biological targets with specific acoustic impedance similar to that of the host fluid, and with dimensions on the order of the acoustic wavelength. This parameter range, combined with the use of standing waves to separate the targets, lends itself to use of the Born approximation for calculating the acoustic radiation force. Considered here is the configuration analyzed by Peng et al. [J. Mech. Phys. Solids 145, 104134 (2020)], in which two intersecting plane waves radiated into the fluid by a standing surface acoustic wave exert a force on a eukaryotic

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5

Du, Liangfen, and Zheng Fan. "Anomalous refraction of acoustic waves using double layered acoustic grating." INTER-NOISE and NOISE-CON Congress and Conference Proceedings 268, no. 6 (2023): 2396–403. http://dx.doi.org/10.3397/in_2023_0353.

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The paper proposes a double layered acoustic grating for fulfilling acoustic focusing in an anomalous direction. The acoustic grating consists of two layers of rigid panels with periodically perforated slits. By optimizing the positions of the slits on the two layers, both positive and negative refractive indices can be achieved with the phase shift tailored within [-π/2, π/2]. This allows acoustic energy of an obliquely incident plane wave to converge in a predefined focusing region in any direction. The paper predicts the wave propagation manipulated by the acoustic grating based on the surf

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6

Sonner, Maximilian M., Farhad Khosravi, Lisa Janker, et al. "Ultrafast electron cycloids driven by the transverse spin of a surface acoustic wave." Science Advances 7, no. 31 (2021): eabf7414. http://dx.doi.org/10.1126/sciadv.abf7414.

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Spin-momentum locking is a universal wave phenomenon promising for applications in electronics and photonics. In acoustics, Lord Rayleigh showed that surface acoustic waves exhibit a characteristic elliptical particle motion strikingly similar to spin-momentum locking. Although these waves have become one of the few phononic technologies of industrial relevance, the observation of their transverse spin remained an open challenge. Here, we observe the full spin dynamics by detecting ultrafast electron cycloids driven by the gyrating electric field produced by a surface acoustic wave propagating

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7

Zhang, Likun, and Zheguang Zou. "Modeling of airborne ultrasound reflection from water surface waves." Journal of the Acoustical Society of America 152, no. 4 (2022): A232. http://dx.doi.org/10.1121/10.0016114.

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Airborne ultrasound reflection from water surface waves is modelled to advance uses of acoustic signals to measure water surface waves and apply the measurements to explore interactions of water waves with rigid structures in a laboratory setting. When the ultrasound is incident on a moving periodic water surface wave, the reflected signal can be treated as diffraction from a moving corrugated reflection grating. Under the condition that the amplitude of the water surface waves is much less than the incident acoustic wavelength, diffraction theory leads to analytical formulas for the spectra o

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8

Noto, Kenichi. "Surface acoustic wave filter, surface acoustic wave device and communication device." Journal of the Acoustical Society of America 122, no. 6 (2007): 3143. http://dx.doi.org/10.1121/1.2822925.

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9

Yokota, Yuuko. "Surface acoustic wave device, surface acoustic wave apparatus, and communications equipment." Journal of the Acoustical Society of America 124, no. 2 (2008): 702. http://dx.doi.org/10.1121/1.2969605.

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10

Baev, A. R., A. L. Mayorov, M. V. Asadchaya, V. N. Levkovich, and K. G. Zhavoronkov. "Features of the Surface and Subsurface Waves Application for Ultrasonic Evaluation of Physicomechanical Properties of Solids. Part 1. Influence of the Geometrical Parameters." Devices and Methods of Measurements 9, no. 4 (2018): 325–26. http://dx.doi.org/10.21122/2220-9506-2018-9-4-325-326.

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Application of surface and subsurface waves for control of objects with a double-layer structure allows to extend possibilities of diagnostics of their physico-mechanical properties. The purpose of work was to determine conditions and offer recommendations providing measuring of ultrasonic velocity and amplitude of the former modes in protective layers and in basis of object at one-sided access to its surface.The analysis of an acoustic path of a measuring system in relation to ultrasonic evaluation of the objects having the restricted sizes and the protective coating according to velocity dat

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11

Shen, Jian Qi. "Canonical Acoustics and Its Application to Surface Acoustic Wave on Acoustic Metamaterials." Journal of the Physical Society of Japan 85, no. 8 (2016): 084401. http://dx.doi.org/10.7566/jpsj.85.084401.

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12

Guo, Lixian, and Dan Zhao. "Enhancing heat-driven acoustic characteristics of standing wave thermoacoustic engines by using corrugated stack." Journal of the Acoustical Society of America 154, no. 4_supplement (2023): A285—A286. http://dx.doi.org/10.1121/10.0023543.

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The present work considers the heat-driven acoustic characteristics and dynamic thermal-fluid flow fields of a standing-wave thermoacoustic engine (SWTAE) by using sinusoidally shaped corrugated stack surfaces. 3-D numerical SWTAE models are developed and validated, aiming to examine the heat-driven acoustic effects caused by different corrugation amplitudes and wave-lengths of the sinusoidal stack surface. The results demonstrate that corrugated-shaped stack channels increase the contact area of the working gas in the stack area, and the thermos-acoustic conversion is more amplified. Compared

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13

Liu, G. R., J. Tani, T. Ohyoshi, and K. Watanabe. "Characteristic Wave Surfaces in Anisotropic Laminated Plates." Journal of Vibration and Acoustics 113, no. 3 (1991): 279–85. http://dx.doi.org/10.1115/1.2930182.

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A numerical method is used to determine the dispersion relation (an eigenvalue equation) of plane wave propagation in an anisotropic laminated plate. A phase velocity surface, phase slowness surface, phase wave surface, group velocity surface, group slowness surface, and group wave surface are defined and their formulae are deduced from the Rayleigh quotient and the orthogonality condition of the eigenvectors of the eigenvalue equation. The six characteristic surfaces can be used to illustrate the characteristics of plane waves and waves generated from a point source in an anisotropic laminate

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14

Zhang, Lihong. "Method of acoustic separation on the surface of cylindrical baffle." Journal of the Acoustical Society of America 154, no. 4_supplement (2023): A356. http://dx.doi.org/10.1121/10.0023786.

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This paper suggests a statistically optimal near-field acoustic holography method based on the combination of plane waves and cylindrical waves, which is used for underwater cylindrical baffles. The method addresses the issue that the extraction of scattered acoustic waves from the surface of underwater cylindrical baffles requires too many measurement points in practical applications: separation of incident and dispersed sound fields and near-field measurements of sound fields at baffle surfaces.The underwater detection sound source is situated in the scatterer's far-field region, so in the a

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15

Lu, Zhiqu. "An acoustic near surface soil profiler using surface wave method." Journal of the Acoustical Society of America 151, no. 4 (2022): A58. http://dx.doi.org/10.1121/10.0010649.

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An acoustic soil profiler, using a so-called the high-frequency multi-channel analysis of surface waves (HF-MASW) method, has been developed, which uses surface (Rayleigh) waves to measure soil profile in terms of the shear (S) wave velocity as a function of depth, up to a 2.5 m deep below the surface. Several practical techniques have been developed to enhance the HF-MASW method, including (1) a variable sensor spacing configuration, (2) the self-adaptive method, and (3) the phase-only signal processing. Fundamentally, the S-wave velocity is related to soil mechanical and hydrological propert

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16

Vetelino, John F. "Surface acoustic wave microsensors." Journal of the Acoustical Society of America 99, no. 4 (1996): 2479–500. http://dx.doi.org/10.1121/1.415570.

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17

Kando, Hajime. "Surface acoustic wave device." Journal of the Acoustical Society of America 122, no. 2 (2007): 696. http://dx.doi.org/10.1121/1.2771304.

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18

Ozaki, Kyosuke. "Surface acoustic wave device." Journal of the Acoustical Society of America 122, no. 2 (2007): 697. http://dx.doi.org/10.1121/1.2771305.

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19

Kidoh, Hideo. "Surface acoustic wave filter." Journal of the Acoustical Society of America 122, no. 2 (2007): 697. http://dx.doi.org/10.1121/1.2771306.

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20

Dwyer, Douglas F. G., and David E. Bower. "Surface acoustic wave accelerometer." Journal of the Acoustical Society of America 82, no. 1 (1987): 409. http://dx.doi.org/10.1121/1.395489.

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21

Kando, Hajime. "Surface acoustic wave device." Journal of the Acoustical Society of America 124, no. 3 (2008): 1389. http://dx.doi.org/10.1121/1.2986167.

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22

Yoneya, Katsuro. "Surface acoustic wave element." Journal of the Acoustical Society of America 124, no. 6 (2008): 3364. http://dx.doi.org/10.1121/1.3047393.

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23

Kam, Chan Hin. "Surface acoustic wave device." Journal of the Acoustical Society of America 124, no. 6 (2008): 3365. http://dx.doi.org/10.1121/1.3047395.

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24

Kadota, Michio. "Surface acoustic wave device." Journal of the Acoustical Society of America 125, no. 2 (2009): 1259. http://dx.doi.org/10.1121/1.3081327.

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25

Kihara, Yoshikazu. "Surface acoustic wave device." Journal of the Acoustical Society of America 126, no. 2 (2009): 927. http://dx.doi.org/10.1121/1.3204322.

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26

Lin, I.-Nan. "Surface acoustic wave substrate." Journal of the Acoustical Society of America 126, no. 2 (2009): 931. http://dx.doi.org/10.1121/1.3204337.

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27

Chen, Ga-Lane. "Surface acoustic wave device." Journal of the Acoustical Society of America 126, no. 5 (2009): 2831. http://dx.doi.org/10.1121/1.3262542.

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28

Wachi, Hirotada. "Surface acoustic wave device." Journal of the Acoustical Society of America 126, no. 6 (2009): 3380. http://dx.doi.org/10.1121/1.3274272.

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29

Sinha, Bikash K., and Michel Gouilloud. "Surface acoustic wave sensors." Journal of the Acoustical Society of America 78, no. 5 (1985): 1932. http://dx.doi.org/10.1121/1.392695.

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30

Miura, Michio. "Surface acoustic wave device." Journal of the Acoustical Society of America 113, no. 4 (2003): 1782. http://dx.doi.org/10.1121/1.1572315.

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31

Kando, Hajime, and Michio Kadota. "Surface acoustic wave device." Journal of the Acoustical Society of America 120, no. 2 (2006): 571. http://dx.doi.org/10.1121/1.2336648.

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32

da Cunha, Mauricio Pereira. "Surface acoustic wave sensor." Journal of the Acoustical Society of America 120, no. 5 (2006): 2397. http://dx.doi.org/10.1121/1.2395087.

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33

Kadota, Michio. "Surface acoustic wave device." Journal of the Acoustical Society of America 120, no. 5 (2006): 2402. http://dx.doi.org/10.1121/1.2395109.

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34

Yamamoto, Koji. "Surface acoustic wave device." Journal of the Acoustical Society of America 120, no. 5 (2006): 2402. http://dx.doi.org/10.1121/1.2395110.

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35

Takamine, Yuichi. "Surface acoustic wave device." Journal of the Acoustical Society of America 120, no. 5 (2006): 2403. http://dx.doi.org/10.1121/1.2395114.

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36

Kalantar-Zadeh, Kourosh, and Wojtek Wlodarski. "Surface acoustic wave sensor." Journal of the Acoustical Society of America 120, no. 5 (2006): 2409. http://dx.doi.org/10.1121/1.2395140.

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37

Bungo, Akihiro. "Surface acoustic wave device." Journal of the Acoustical Society of America 121, no. 1 (2007): 16. http://dx.doi.org/10.1121/1.2434272.

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38

Noguchi, Hitoshi, and Yoshihiro Kubota. "Surface acoustic wave device." Journal of the Acoustical Society of America 121, no. 4 (2007): 1834. http://dx.doi.org/10.1121/1.2723997.

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39

Nysen, Paul A., and Halvor Skeie. "Surface acoustic wave modulator." Journal of the Acoustical Society of America 121, no. 5 (2007): 2482. http://dx.doi.org/10.1121/1.2739145.

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40

Kando, Hajime. "Surface acoustic wave device." Journal of the Acoustical Society of America 121, no. 5 (2007): 2482. http://dx.doi.org/10.1121/1.2739146.

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41

Yamanouchi, Kazuhiko. "Surface acoustic wave transducer." Journal of the Acoustical Society of America 121, no. 5 (2007): 2483. http://dx.doi.org/10.1121/1.2739147.

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42

Hada, Takuo. "Surface acoustic wave device." Journal of the Acoustical Society of America 121, no. 5 (2007): 2483. http://dx.doi.org/10.1121/1.2739148.

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43

LINTON, C. M., and M. McIVER. "The existence of Rayleigh–Bloch surface waves." Journal of Fluid Mechanics 470 (October 31, 2002): 85–90. http://dx.doi.org/10.1017/s0022112002002227.

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Rayleigh–Bloch surface waves arise in many physical contexts including water waves and acoustics. They represent disturbances travelling along an infinite periodic structure. In the absence of any existence results, a number of authors have previously computed such modes for certain specific geometries. Here we prove that such waves can exist in the absence of any incident wave forcing for a wide class of structures.

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44

Yves, Simon, Yu-Gui Peng, and Andrea Alù. "Topological Lifshitz transition in twisted hyperbolic acoustic metasurfaces." Applied Physics Letters 121, no. 12 (2022): 122201. http://dx.doi.org/10.1063/5.0107465.

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Acoustic metamaterials and metasurfaces have been explored in the past few years to realize a wide range of extreme responses for sound waves. As one remarkable phenomenon, extreme anisotropy and hyperbolic sound propagation are particularly challenging to realize compared to electromagnetic waves because of the scalar nature of airborne acoustics. In parallel, moiré superlattices and the rapidly expanding domain of twistronics have shown that large anisotropy combined with tailored geometrical rotations can enable tantalizing emerging phenomena, such as tailored phase transitions in metamater

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45

Yoneya, Katsuro. "Surface acoustic wave filter and surface acoustic wave resonator having bent electrode fingers." Journal of the Acoustical Society of America 120, no. 5 (2006): 2402. http://dx.doi.org/10.1121/1.2395112.

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46

Yang, Yang, Corinne Dejous, and Hamida Hallil. "Trends and Applications of Surface and Bulk Acoustic Wave Devices: A Review." Micromachines 14, no. 1 (2022): 43. http://dx.doi.org/10.3390/mi14010043.

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The past few decades have witnessed the ultra-fast development of wireless telecommunication systems, such as mobile communication, global positioning, and data transmission systems. In these applications, radio frequency (RF) acoustic devices, such as bulk acoustic waves (BAW) and surface acoustic waves (SAW) devices, play an important role. As the integration technology of BAW and SAW devices is becoming more mature day by day, their application in the physical and biochemical sensing and actuating fields has also gradually expanded. This has led to a profusion of associated literature, and

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47

Cormack, John M., Yurii A. Ilinskii, Evgenia A. Zabolotskaya, and Mark F. Hamilton. "Nonlinear piezoelectric surface acoustic waves." Journal of the Acoustical Society of America 151, no. 3 (2022): 1829–46. http://dx.doi.org/10.1121/10.0009770.

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The theory for nonlinear surface acoustic waves in crystals developed using Hamiltonian mechanics [Hamilton, Il'inskii, and Zabolotskaya, J. Acoust. Soc. Am. 105, 639 (1999)] is modified to account for piezoelectric material properties. The derived spectral evolution equations permit analysis of nonlinear surface wave propagation along a cut surface of any orientation with respect to the crystallographic axes and for piezoelectric crystals with any symmetry. Numerical simulations of waveform distortion in the particle velocity and electric field components are presented for surface wave propag

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48

Malocha, Donald C. "Surface acoustic wave device fabrication." Journal of the Acoustical Society of America 99, no. 4 (1996): 2479–500. http://dx.doi.org/10.1121/1.415569.

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49

Soltie, Leland P. "Surface acoustic wave Doppler detector." Journal of the Acoustical Society of America 88, no. 4 (1990): 2051. http://dx.doi.org/10.1121/1.400122.

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50

Takasaki, Masaya. "Surface acoustic wave excitation device." Journal of the Acoustical Society of America 126, no. 2 (2009): 931. http://dx.doi.org/10.1121/1.3204338.

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