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Journal articles on the topic 'Surface acoustics wave'

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Published: 8 June 2024

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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 (November 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

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 (April 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 cell modeled as a multilayered sphere. The angle of intersection is determined by the velocity of the surface wave and the sound speed in the fluid. The acoustic field in this case is a standing wave parallel to the substrate and a traveling wave perpendicular to the substrate. For all parameter values considered by Peng et al., including spheres several wavelengths in diameter, the Born approximation of the acoustic radiation force parallel to the substrate is in good agreement with a full theory based on spherical wave expansions of the incident and scattered fields. [C.A.G. and T.S.J. were supported by ARL:UT McKinney Fellowships in Acoustics.]

4

Sonner, Maximilian M., Farhad Khosravi, Lisa Janker, Daniel Rudolph, Gregor Koblmüller, Zubin Jacob, and Hubert J. Krenner. "Ultrafast electron cycloids driven by the transverse spin of a surface acoustic wave." Science Advances 7, no. 31 (July 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 on a slab of lithium niobate. A tubular quantum well wrapped around a nanowire serves as an ultrafast sensor tracking the full cyclic motion of electrons. Our acousto-optoelectrical approach opens previously unknown directions in the merged fields of nanoacoustics, nanophotonics, and nanoelectronics for future exploration.

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 (November 30, 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 surface coupling approach. Then, it discusses how to optimize the slits' positions to collimate the acoustic energy of an obliquely incident plane wave in a specific direction. Such acoustic grating has various potential applications, such as deflecting outdoor noise away from sensitive areas in building acoustics, enhancing acoustic energy in a target audience area in auditorium design, collimating acoustic surface waves, etc.

6

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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7

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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8

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 (August 15, 2016): 084401. http://dx.doi.org/10.7566/jpsj.85.084401.

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9

Zhang, Likun, and Zheguang Zou. "Modeling of airborne ultrasound reflection from water surface waves." Journal of the Acoustical Society of America 152, no. 4 (October 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 of the acoustic signal relating to the water wave amplitudes and frequencies. Complementary modeling based on ray theory and wave superposition illustrates the diffraction and validates formulas of water wave reflection from a surface-piercing barrier structure, where two counter-propagating water waves are involved.

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 (December 17, 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 data of the surface and subsurface waves propagation is made. On the basis of representations of beam acoustics the dependences connecting a wavelength of the excited surface and subsurface modes, thickness and width of a controlled object, acoustic base of a sounding are defined. There are to provide a condition leveling of the influence of an acoustical noise created by the reflected and accompanying waves on parameters of acoustic signal with the given quantity of oscillations in an impulse.The principle opportunity is shown and conditions for determination of velocity of subsurface body waves in the base material which is under a protective coating layer are established. For these purposes on the basis of use of the block of ultrasonic probes the optimum scheme of a sounding is offered and the analytical expression for calculation of required velocity considering varying of thickness of a covering is received.The method of acoustical measuring realized by a direct and reverse sounding of the objects with small aperture and angle probes was analysed and formulas for determination of speed of subsurface wave under protective layer of the wedge form have been got. An ultrasonic device is suggested for the excitationreception of subsurface waves with different speed in objects (on 20–35 %) using for the acoustic concordance of environments of metallic sound duct as a wedge. Possibility of leveling of interference in a protective layer to control efects in basis of material by a volume wave by creation of supporting echo-signal of longitudinal wave of the set frequency and entered normally to the surface of object was studied.

11

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

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12

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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13

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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14

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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15

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

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16

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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17

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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18

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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19

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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20

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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21

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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22

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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23

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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24

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

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25

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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26

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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27

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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28

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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29

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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30

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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31

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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32

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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33

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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34

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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35

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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36

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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37

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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38

Lu, Zhiqu. "An acoustic near surface soil profiler using surface wave method." Journal of the Acoustical Society of America 151, no. 4 (April 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 properties through the principle of effective stress. Therefore, the measured two-dimensional S-wave velocity images reflect the temporal and spatial variations of soils due to weather effects, geological anomalies, and anthropologic activities. Several HF-MASW applications will be reported, including (1) near surface soil profiling, (2) a long-term-survey for studying weather and seasonal effects, (3) short-term monitoring rain fall events, (4) detecting fraigpan layers, and (5) a farmland compaction study. This acoustic soil profiler can be used for agricultural, environmental, civil engineering, and military applications.

39

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 (July 1, 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 laminated plate. As numerical examples, the characteristic surfaces are computed for graphite/epoxy angle ply laminated plates and for a hybrid one. The results for the graphite/epoxy laminated plates are compared with those obtained by Moon’s approximate theory.

40

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 (October 1, 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 to the SWTAE with uniform-shaped stack, the corrugated-shaped stack exhibit enhanced acoustic power output while maintaining a constant acoustic oscillation frequency. With the corrugation peak and wave-length of the sinusoidal stack are 2 and 0.2 mm, respectively, the amplitude and acoustic power of the acoustic pressure oscillations increase by 10.12% and 17.31%, respectively, in comparison with that of the conventional SWTAE. However, when the corrugation peak exceeds 0.4 mm, stronger nonlinear acoustics and flow effects are observed in the stack channels, leading to a reduction in the heat-driven acoustic power output, and thermo-acoustics energy conversion efficiency. The developed model highlights the effects of the corrugated-shaped stack on enhancing acoustic power output and thermo-acoustic conversion efficiency.

41

Zhang, Lihong. "Method of acoustic separation on the surface of cylindrical baffle." Journal of the Acoustical Society of America 154, no. 4_supplement (October 1, 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 actual application scenario for the surface acoustic scattering separation of the cylindrical baffle, the plane wave expansion is used to represent the surface incident acoustic wave and the cylindrical wave expansion is used to describe the scattered acoustic wave on the baffle surface. As a result, fewer expansion orders are required to describe the entire sound field on the baffle's surface. It is verified by simulation that the method is valid and efficient for near-field total sound field measurement and dispersed sound field separation of roughly cylindrical targets under underwater far-field incidence situations because the measurement holographic surface of the surface permits unlimited geometries.

42

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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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.

44

Yves, Simon, Yu-Gui Peng, and Andrea Alù. "Topological Lifshitz transition in twisted hyperbolic acoustic metasurfaces." Applied Physics Letters 121, no. 12 (September 19, 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 metamaterials. Connecting these areas of research, here, we explore the realization of acoustic hyperbolic metasurfaces and their combination to drive topological phase transitions from hyperbolic to elliptic sound propagation. The transition point occurring at a specific rotation angle between two acoustic metasurfaces supports highly directional canalization of sound, opening exciting opportunities for twisted acoustics metasurfaces for robust surface wave guiding and steering.

45

Yang, Yang, Corinne Dejous, and Hamida Hallil. "Trends and Applications of Surface and Bulk Acoustic Wave Devices: A Review." Micromachines 14, no. 1 (December 24, 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 this article particularly aims to help young professionals and students obtain a comprehensive overview of such acoustic technologies. In this perspective, we report and discuss the key basic principles of SAW and BAW devices and their typical geometries and electrical characterization methodology. Regarding BAW devices, we give particular attention to film bulk acoustic resonators (FBARs), due to their advantages in terms of high frequency operation and integrability. Examples illustrating their application as RF filters, physical sensors and actuators, and biochemical sensors are presented. We then discuss recent promising studies that pave the way for the exploitation of these elastic wave devices for new applications that fit into current challenges, especially in quantum acoustics (single-electron probe/control and coherent coupling between magnons and phonons) or in other fields.

46

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

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47

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

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48

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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49

Morimoto, Mikio. "Surface acoustic wave bandpass filter." Journal of the Acoustical Society of America 77, no. 6 (June 1985): 2210. http://dx.doi.org/10.1121/1.391658.

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50

To, Yasushi Yamamo. "Surface acoustic wave resonator filter." Journal of the Acoustical Society of America 113, no. 4 (2003): 1781. http://dx.doi.org/10.1121/1.1572314.

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