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Search Results (421)

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Keywords = acoustic wave device

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11 pages, 3029 KiB  
Article
Laterally Excited Resonators Based on Single-Crystalline LiTaO3 Thin Film for High-Frequency Applications
by Chongrui Guan and Xingli He
Micromachines 2024, 15(12), 1416; https://doi.org/10.3390/mi15121416 - 26 Nov 2024
Viewed by 257
Abstract
High-performance acoustic resonators based on single-crystalline piezoelectric thin films have great potential in wireless communication applications. This paper presents the modeling, fabrication, and characterization of laterally excited bulk resonators (XBARs) utilizing the suspended ultra-thin (~420 nm) LiTaO3 (LT, with 42° YX-cut) film. [...] Read more.
High-performance acoustic resonators based on single-crystalline piezoelectric thin films have great potential in wireless communication applications. This paper presents the modeling, fabrication, and characterization of laterally excited bulk resonators (XBARs) utilizing the suspended ultra-thin (~420 nm) LiTaO3 (LT, with 42° YX-cut) film. The finite element analysis (FEA) was performed to model the LT-based XBARs precisely and to gain further insight into the physical behaviors of the acoustic waves and the loss mechanisms. In addition, the temperature response of the devices was numerically calculated, showing relatively low temperature coefficients of frequency (TCF) of ~−38 ppm/K for the primary resonant mode. The LT-based XBARs were fabricated and characterized, which presents a multi-resonant mode over a wide frequency range (0.1~10 GHz). For the primary resonance around 4.1 GHz, the fabricated devices exhibited a high-quality factor (Bode-Q) ~ 600 and piezoelectric coupling (kt2) ~ 2.84%, while the higher-harmonic showed a greater value of kt2 ~ 3.49%. To lower the resonant frequency of the resonator, the thin SiO2 film (~20 nm) was sputtered on the suspended device, which created a frequency offset between the series and shunt resonators. Finally, a ladder-type narrow band filter employing five XBARs was developed and characterized. This work effectively demonstrates the performance and application potential of micro-acoustic resonators employing high-quality LT films. Full article
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<p>(<b>a</b>) Fabrication process flow of LT-based XBARs; (<b>b</b>) SEM image of the resonator before etching the back trench; (<b>c</b>) zoom-in image showing the width of finger pairs; microscope images of the device with a back view (<b>d</b>) and a top view (<b>e</b>).</p>
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<p>(<b>a</b>) 3D geometry of the proposed plate wave resonator using LT thin film with meshed domains, displaying the finite element distribution; the geometry scale is magnified 20 times along the thickness of the thin plate for easier discernment. (<b>b</b>) Comparison of the impedance characteristics between the accurate 3D FEM models and experimental results.</p>
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<p>COMSOL simulation results show the displacement mode shape of the device around the primary resonance; the upper image depicts the displacement mode shape of the truncated strip comprising one finger pair.</p>
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<p>The comparison of the SAW velocities in a bulk crystal and a thin crystalline film of LiTaO<sub>3</sub>.</p>
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<p>Comparison of the impedances of LT thin film-based acoustic resonators under different temperatures.</p>
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<p>(<b>a</b>) The measured admittance (Y<sub>11</sub>) spectrum of the resonator over a wide frequency range. (<b>b</b>) The calculated Bode-Q of the resonator near the primary resonance.</p>
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<p>(<b>a</b>) Microscopy image of the prepared ladder-type filter; the admittance for representative one-port resonator to compose the series (<b>b</b>) and shunt (<b>c</b>) branch of the filter; (<b>d</b>) frequency response of the LT-plate-based filter over a wide frequency range, where the zoom-in images of the transmission (S<sub>21</sub>) and return loss (S<sub>11</sub>) of the filter in the vicinity of the passband was inserted.</p>
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17 pages, 12577 KiB  
Article
Acoustic Tunnel Lining Void Detection: Modeling and Instrument System Development
by Luxin Tang, Jinbin Zeng, Chuixin Chen, Jian Huang, Shuxing Zhou, Li Wang, Defu Zhang, Weibin Wu and Ting Gao
Processes 2024, 12(12), 2651; https://doi.org/10.3390/pr12122651 - 25 Nov 2024
Viewed by 397
Abstract
The detachment of railway tunnel lining constitutes a grave danger to train operation safety and drastically curtails the tunnel’s service life. This study endeavors to efficiently detect the void defects in railway tunnel lining by creating a finite element model of tunnel lining [...] Read more.
The detachment of railway tunnel lining constitutes a grave danger to train operation safety and drastically curtails the tunnel’s service life. This study endeavors to efficiently detect the void defects in railway tunnel lining by creating a finite element model of tunnel lining structures. Utilizing this model, the study simulates the nonlinear acoustic wave propagation cloud maps for three representative tunnel lining structures: void-free, air void, and water void. This facilitates a thorough examination of the acoustic signal characteristics in the wavefield, time domain, and frequency domain. To satisfy the precision and efficiency demands of tunnel lining void detection, this study has devised and developed a portable acoustic detector that incorporates automatic analysis and processing capabilities and is furnished with a high-performance rare-earth magneto-strictive acoustic excitation device. This detection system can swiftly detect and assess typical void defects in tunnel lining. To further validate the effectiveness of this system, this study conducted lining defect detection in the Pingdao Railway Tunnel in the eastern Qinling Mountains. The test results show that the detection rate of this system for both air-filled and water-filled voids with a width of 1 m reached 100%, demonstrating its extremely high application value. Full article
(This article belongs to the Section Manufacturing Processes and Systems)
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<p>Tunnel concrete lining structure.</p>
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<p>Finite element geometric model diagram of tunnel concrete lining voiding structure.</p>
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<p>Mesh generation diagram of the finite element model for lining void structure.</p>
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<p>Scenes at the tunnel entrance.</p>
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<p>Scenes inside the tunnel.</p>
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<p>Schematic diagram of surveyed cross-section.</p>
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<p>Cloud diagrams of sound wave propagation at different times in non-void lining structures.</p>
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<p>Cloud diagrams of sound wave propagation at different times in air void lining structures.</p>
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<p>Cloud diagrams of Sound Wave Propagation at Different Times in Water-Filled Void Lining Structures.</p>
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<p>Waveform diagram of acoustic wave time-domain signal for tunnel lining void structure.</p>
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<p>Waveform diagram of acoustic wave time-domain signal for tunnel lining void structure.</p>
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<p>Time-domain reflected echo energy diagram of tunnel lining structure.</p>
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<p>Relationship diagram of time-domain reflected echo energy ratio versus void width <span class="html-italic">L</span>.</p>
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<p>Waveform diagram of acoustic wave frequency-domain signals for void-containing tunnel lining structures.</p>
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<p>Waveform diagram of acoustic wave frequency-domain signals for void-containing tunnel lining structures.</p>
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<p>Reflection echo energy ratio of frequency-domain signals for tunnel lining structures.</p>
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<p>Relationship diagram of frequency-domain reflected echo energy ratio versus void width <span class="html-italic">L</span>.</p>
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<p>Schematic diagram of acoustic wave detection system for void detection in lining structures.</p>
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<p>Principle and structural diagram of rare-earth giant MLT.</p>
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<p>Rare-earth giant MLT component.</p>
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<p>Test results for non-void area model.</p>
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<p>Test results for non-void area model.</p>
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<p>Test results for the model of water-filled void area.</p>
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14 pages, 3443 KiB  
Article
Acoustic Communication Among Smart Sensors: A Feasibility Study
by Paolo Caruso, Helbert da Rocha, Antonio Espírito-Santo, Vincenzo Paciello and José Salvado
Instruments 2024, 8(4), 51; https://doi.org/10.3390/instruments8040051 - 22 Nov 2024
Viewed by 327
Abstract
Smart sensors and networks have spread worldwide over the past few decades. In the industry field, these concepts have found an increasing quantity of applications. The omnipresence of smart sensor networks and smart devices, especially in the industrial world, has contributed to the [...] Read more.
Smart sensors and networks have spread worldwide over the past few decades. In the industry field, these concepts have found an increasing quantity of applications. The omnipresence of smart sensor networks and smart devices, especially in the industrial world, has contributed to the emergence of the concept of Industry 4.0. In a world where everything is interconnected, communication among smart devices is critical to technological development in the field of smart industry. To improve communication, many engineers and researchers implemented methods to standardize communication along the various levels of the ISO-OSI model, from hardware design to the implementation and standardization of different communication protocols. The objective of this paper is to study and implement an unconventional type of communication, exploiting acoustic wave propagation on metallic structures, starting from the state of the art, and highlighting the advantages and disadvantages found in existing literature, trying to overcome them and describing the progress beyond the state of the art. The proposed application for acoustic communication targets the field of smart industries, where implementing signal transmission via wireless or wired methods is challenging due to interference from the widespread presence of metallic structures. This study explores an innovative approach to acoustic communication, with a particular focus on the physical challenges related to acoustic wave propagation. Additionally, communication performance is examined in terms of noise rejection, analyzing the impact of injected acoustic noise on communication efficiency. Full article
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<p>Simulation results of the frequency response for the 70 cm- (black curve), 140 cm- (blue curve), and 280 cm-long (red curve) aluminum bars.</p>
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<p>Frequency response of the communication system.</p>
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<p>Schematic diagram of the noise measurement experiment.</p>
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<p>Results of the noise profile analysis.</p>
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<p>Trend over time of the Vout duty cycle “D”.</p>
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<p>Custom-made PCB with two layers: (<b>a</b>) modulation layer; (<b>b</b>) demodulation layer.</p>
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<p>Experimental setup for acoustic communication.</p>
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<p>Experimental setup for acoustic communication.</p>
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<p>Frequency vs. packet loss at various noise amplitude levels.</p>
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21 pages, 2927 KiB  
Review
MHD Generation for Sustainable Development, from Thermal to Wave Energy Conversion: Review
by José Carlos Domínguez-Lozoya, David Roberto Domínguez-Lozoya, Sergio Cuevas and Raúl Alejandro Ávalos-Zúñiga
Sustainability 2024, 16(22), 10041; https://doi.org/10.3390/su162210041 - 18 Nov 2024
Viewed by 676
Abstract
Magnetohydrodynamic (MHD) generators are direct energy conversion devices that transform the motion of an electrically conducting fluid into electricity through interaction with a magnetic field. Developed as an alternative to conventional turbine-generator systems, MHD generators evolved through the 20th century from large units, [...] Read more.
Magnetohydrodynamic (MHD) generators are direct energy conversion devices that transform the motion of an electrically conducting fluid into electricity through interaction with a magnetic field. Developed as an alternative to conventional turbine-generator systems, MHD generators evolved through the 20th century from large units, which are intended to transform thermal energy into electricity using plasma as a working fluid, to smaller units that can harness heat from a variety of sources. In the last few decades, an effort has been made to develop energy conversion systems that incorporate MHD generators to harvest renewable sources such as solar and ocean energy, strengthening the sustainability of this technology. This review briefly synthesizes the main steps in the evolution of MHD technology for electricity generation, starting by outlining its physical principles and the proposals to convert thermal energy into electricity, either using a high-temperature plasma as a working fluid or a liquid metal in a one- or two-phase flow at lower temperatures. The use of wave energy in the form of acoustic waves, which were obtained from the conversion of thermal energy through thermoacoustic devices coupled to liquid metal and plasma MHD generators, as well as alternatives for the transformation of environmental energy resources employing MHD transducers, is also assessed. Finally, proposals for the conversion of ocean energy, mainly in the form of waves and tides, into electric energy, through MHD generators using either seawater or liquid metal as working fluids, are presented along with some of the challenges of MHD conversion technology. Full article
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<p>Faraday MHD electric generator with constant cross-section for incompressible working fluid (<b>a</b>) and with variable cross-section for compressible working fluid (<b>b</b>).</p>
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<p>MHD system for direct conversion of heat to electricity with natural circulation using a lead–bismuth alloy, operating in a temperature range of 338–423 K. Developed in the ETGAR Program [<a href="#B36-sustainability-16-10041" class="html-bibr">36</a>,<a href="#B37-sustainability-16-10041" class="html-bibr">37</a>].</p>
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<p>Schematic illustration of a liquid metal MHD thermoacoustic generator with two prime movers [<a href="#B10-sustainability-16-10041" class="html-bibr">10</a>].</p>
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<p>Sketch of a WEC coupled to an LMMHD generator using a double-acting piston system with a working fluid and a neoprene bellow that drives the liquid metal [<a href="#B96-sustainability-16-10041" class="html-bibr">96</a>]. A similar system can operate with multiple coupled devices [<a href="#B99-sustainability-16-10041" class="html-bibr">99</a>].</p>
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<p>Laboratory scale of a conductive alternate liquid metal MHD generator [<a href="#B109-sustainability-16-10041" class="html-bibr">109</a>].</p>
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13 pages, 5902 KiB  
Article
Modulation of Surface Elastic Waves and Surface Acoustic Waves by Acoustic–Elastic Metamaterials
by Chang Fu and Tian-Xue Ma
Crystals 2024, 14(11), 997; https://doi.org/10.3390/cryst14110997 - 18 Nov 2024
Viewed by 466
Abstract
Metamaterials enable the modulation of elastic waves or acoustic waves in unprecedented ways and have a wide range of potential applications. This paper achieves the simultaneous manipulation of surface elastic waves (SEWs) and surface acoustic waves (SAWs) using two-dimensional acousto-elastic metamaterials (AEMMs). The [...] Read more.
Metamaterials enable the modulation of elastic waves or acoustic waves in unprecedented ways and have a wide range of potential applications. This paper achieves the simultaneous manipulation of surface elastic waves (SEWs) and surface acoustic waves (SAWs) using two-dimensional acousto-elastic metamaterials (AEMMs). The proposed AEMMs are composed of periodic hollow cylinders on the surface of a semi-infinite substrate. The band diagrams and the frequency responses of the AEMMs are numerically calculated through the finite element approach. The band diagrams exhibit simultaneous bandgaps for the SEWs and SAWs, which can also be effectively tuned by the modification of AEMM geometry. Furthermore, we construct the AEMM waveguide by the introduction of a line defect and hence demonstrate its ability to guide the SEWs and SAWs simultaneously. We expect that the proposed AEMMs will contribute to the development of multi-functional wave devices, such as filters for dual waves in microelectronics or liquid sensors that detect more than one physical property. Full article
(This article belongs to the Section Hybrid and Composite Crystalline Materials)
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<p>Schemes of the AEMM unit cells for the elastic (<b>a</b>) and acoustic (<b>b</b>) waves. (<b>c</b>) Cross-section view of the AEMM unit cell. (<b>d</b>) The first Brillouin zone of the square lattice.</p>
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<p>Band diagrams of the AEMM unit cell for the elastic (<b>a</b>) and acoustic (<b>b</b>) waves. (<b>c</b>) Displacement distributions and deformations of the SEW modes marked in (<b>a</b>). (<b>d</b>) Pressure distributions of the SAW modes marked in (<b>b</b>).</p>
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<p>Transmission spectra of the SEWs (<b>a</b>) and SAWs (<b>b</b>) in the finite-sized AEMM along the <math display="inline"><semantics> <mi mathvariant="normal">Γ</mi> </semantics></math>X direction.</p>
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<p>Distributions of the displacement (<b>a</b>) and pressure (<b>b</b>) fields of the finite-sized AEMM at different excitation frequencies.</p>
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<p>Band diagrams of the AEMM unit cell with different cylinder heights, where the upper and lower panels are the results of the elastic and acoustic waves, respectively.</p>
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<p>Transmission curves of the SEWs (<b>upper panel</b>) and SAWs (<b>lower panel</b>) along the <math display="inline"><semantics> <mi mathvariant="normal">Γ</mi> </semantics></math>X direction for different cylinder heights.</p>
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<p>Schemes of the AEMM supercells with a line defect for the elastic (<b>a</b>) and acoustic (<b>b</b>) waves.</p>
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<p>Band diagrams of the AEMM supercell for the elastic (<b>a</b>) and acoustic (<b>b</b>) waves, where the direction of wave propagation is the <math display="inline"><semantics> <mi mathvariant="normal">Γ</mi> </semantics></math>X direction.</p>
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<p>(<b>a</b>) Displacement distributions and deformations of the SEW modes marked in <a href="#crystals-14-00997-f008" class="html-fig">Figure 8</a>a. (<b>b</b>) Pressure distributions of the SAW modes marked in <a href="#crystals-14-00997-f008" class="html-fig">Figure 8</a>b.</p>
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<p>Schemes for calculating the frequency responses of the AEMM waveguide: (<b>a</b>) solid domain and (<b>b</b>) air domain.</p>
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<p>(<b>a</b>) Transmission curves of the SEWs in the AEMM waveguide, where the normalized frequencies corresponding to marker points 1, 2 are 0.257, 0.293. (<b>b</b>) Transmission curves of the SAWs in the AEMM waveguide, where the normalized frequencies corresponding to marker points I, II are 0.30, 0.36.</p>
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<p>Distributions of the displacement (<b>a</b>) and pressure (<b>b</b>) fields of the AEMM waveguide at different excitation frequencies.</p>
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12 pages, 4205 KiB  
Article
Design of Acoustic Absorbing Structures for Mercurous Halide-Based Acousto-Optic Tunable Filters
by Shujing Sun, Huijie Zhao, Qi Guo and Yijie Wang
Materials 2024, 17(22), 5606; https://doi.org/10.3390/ma17225606 - 16 Nov 2024
Viewed by 358
Abstract
For the acousto-optic tunable filter (AOTF)-based spectral imaging systems, the diffraction efficiency of the AOTF is a primary factor affecting system throughput. Moreover, the distribution of the acoustic field within the AOTF fundamentally determines the device’s diffraction efficiency. Thus, the design of an [...] Read more.
For the acousto-optic tunable filter (AOTF)-based spectral imaging systems, the diffraction efficiency of the AOTF is a primary factor affecting system throughput. Moreover, the distribution of the acoustic field within the AOTF fundamentally determines the device’s diffraction efficiency. Thus, the design of an AOTF device including a transducer and absorber to achieve a uniform acoustic field distribution plays an important role in improving diffraction efficiency. This study proposed an acoustic absorbing structure using mercurous halide crystals’ strong acoustic anisotropy to realize the conversion from shear horizontal wave to surface wave at the boundary and rapid dissipation. Snell’s law for acoustically anisotropic media is employed to design the angle of the acoustic absorbing structure. Experiments of mercurous halide-based AOTF demonstrate that this absorbing structure can effectively enhance diffraction efficiency. Full article
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<p>(<b>a</b>) AOTF three-dimensional structure diagram; (<b>b</b>) a sectional view of the dashed line position in the AOTF three-dimensional diagram.</p>
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<p>(<b>a</b>) Schematic diagram of the Poynting vector direction; (<b>b</b>) slowness curves in the XZ plane for TeO<sub>2</sub>, Hg<sub>2</sub>Br<sub>2</sub>, and Hg<sub>2</sub>Cl<sub>2</sub>; (<b>c</b>) acoustic walk-off angles for TeO<sub>2</sub>, Hg<sub>2</sub>Br<sub>2</sub>, and Hg<sub>2</sub>Cl<sub>2</sub> at different angles.</p>
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<p>(<b>a</b>) The schematic diagram of the reflected wave energy returning to the crystal interior; (<b>b</b>) the schematic diagram of the reflected wave energy propagating along the boundary; (<b>c</b>) the diagram illustrating the principle of Snell’s law at the interface.</p>
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<p>(<b>a</b>) The distribution diagram of the group velocity reflection angle of TeO<sub>2</sub>; (<b>b</b>) the distribution diagram of the group velocity reflection angle of Hg<sub>2</sub>Br<sub>2</sub>; (<b>c</b>) the distribution diagram of the group velocity reflection angle of Hg<sub>2</sub>Cl<sub>2</sub>.</p>
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<p>(<b>a</b>) Acoustic transmission and absorption diagram; (<b>b</b>) diagram of acoustic wave propagation through two crystals.</p>
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<p>(<b>a</b>) Transmission coefficient distribution of Hg<sub>2</sub>Br<sub>2</sub> with Hg<sub>2</sub>Br<sub>2</sub>, Hg<sub>2</sub>Cl<sub>2</sub>, and TeO<sub>2</sub>; (<b>b</b>) phase velocity/transmission angle distribution curves for Hg<sub>2</sub>Br<sub>2</sub>, Hg<sub>2</sub>Cl<sub>2</sub>, and TeO<sub>2</sub>.</p>
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<p>(<b>a</b>) Acoustic-optical diffraction test optical path diagram. P is the polarizer, BE is the beam expander, A is the aperture, RF is the radio frequency signal, I<sub>t</sub> is the transmitted image, I<sub>d</sub> is the diffracted image, LS is the light screen, and CCD is the charge-coupled device; (<b>b</b>) measured images of transmitted and diffracted images; (<b>c</b>) the photograph of the tested Hg<sub>2</sub>Br<sub>2</sub> AOTF.</p>
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<p>(<b>a</b>) The simulation diagram of the amplitude distribution of the acoustic field in mercuric bromide without absorber materials; (<b>b</b>) the simulation diagram of the amplitude distribution of the acoustic field in mercuric bromide with absorber materials; (<b>c</b>) the variation curves of single-point diffraction efficiency before and after the application of adhesive absorber materials with increasing power. Simulation Curves 1 and 2 represent simulation results, while Experimental Data 1 and 2 represent measured results; (<b>d</b>) the variation curves of image diffraction efficiency before and after the application of adhesive absorber materials with increasing power. Simulation Curves 1 and 2 represent simulation results, while Experimental Data 1 and 2 represent measured results.</p>
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9 pages, 4045 KiB  
Article
A Laterally Excited Bulk Acoustic Wave Resonator Based on LiNbO3 with Arc-Shaped Electrodes
by Jieyu Liu, Wenjuan Liu, Zhiwei Wen, Min Zeng and Chengliang Sun
Micromachines 2024, 15(11), 1367; https://doi.org/10.3390/mi15111367 - 12 Nov 2024
Viewed by 541
Abstract
High frequency and large bandwidth are growing trends in communication radio-frequency devices. The LiNbO3 thin film material is expected to become the preferred piezoelectric material for high coupling resonators in the 5G frequency band due to its ultra-high piezoelectric coefficient and low [...] Read more.
High frequency and large bandwidth are growing trends in communication radio-frequency devices. The LiNbO3 thin film material is expected to become the preferred piezoelectric material for high coupling resonators in the 5G frequency band due to its ultra-high piezoelectric coefficient and low loss characteristics. The main mode of laterally excited bulk acoustic wave resonators (XBAR) have an ultra-high sound velocity, which enables high-frequency applications. However, the interference of spurious modes is one of the main reasons hindering the widespread application of XBAR. In this paper, a Z-cut LiNbO3 thin film-based XBAR with arc-shaped electrodes is presented. We investigate the electric field distribution of the XBAR, while the irregular boundary of the arc-shaped electrodes affects the electric field between the existing interdigital transducers (IDTs). The mode shapes and impedance response of the XBAR with arc-shaped electrodes and the XBARs with traditional IDTs are compared in this work. The fabricated XBAR on a 350 nm Z-cut LiNbO3 thin film with arc-shaped electrodes operating at over 5 GHz achieves a high effective electromechanical coupling coefficient of 29.8% and the spurious modes are well suppressed. This work promotes an XBAR with an optimized electrode design to further achieve the desired performance. Full article
(This article belongs to the Special Issue Piezoelectric Devices and System in Micromachines)
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<p>Two-dimensional cross-sectional view of XBARs (<b>a</b>) with IDT electrodes and (<b>b</b>) with arc-shaped electrodes. (<b>c</b>) The cross-sectional view of a XBAR based on a Z-cut LiNbO<sub>3</sub> thin film.</p>
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<p>(<b>a</b>) The schematic of hexagonal unit cell of Z-cut LiNbO<sub>3</sub>. Dispersive diagrams for propagation on the x-axis for the real part of propagation constant (<b>b</b>) while the frequency domain is 0.1–3.5 GHz, (<b>c</b>) while the frequency domain is 3.5–5.5 GHz and (<b>d</b>) while the frequency domain is 5.5–6.5 GHz. (<b>e</b>) The total displacements of different mode shapes while kx = 0 (1/m).</p>
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<p>Process flows of XBAR: (<b>a</b>) The schematic diagram of LNOI wafer. (<b>b</b>) Definition of top electrode. (<b>c</b>) DRIE back surface Si. (<b>d</b>) Suspend the resonator using BOE.</p>
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<p>The microscope images of (<b>a</b>) device with IDT electrodes and (<b>b</b>) device with arc-shaped electrodes.</p>
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<p>The SEM pictures of the fabricated XBARs (<b>a</b>) with arc-shaped electrodes and (<b>b</b>) with IDT electrodes. Measured impedance responses of XBARs (<b>c</b>) with arc-shaped electrodes and (<b>d</b>) with IDT electrodes.</p>
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<p>Simulated impedance curve of XBARs (<b>a</b>) with IDT electrodes and (<b>b</b>) with arc-shaped electrodes.</p>
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<p>Schematic diagram of acoustic wave propagation between adjacent (<b>a</b>) IDT electrodes and (<b>b</b>) arc-shaped electrodes. Simulated electric field distributions of XBARs (<b>c</b>) with IDT electrodes and (<b>d</b>) with arc-shaped electrodes.</p>
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<p>Impedance curve of arc-shaped electrode XBAR when a = 10 μm and (<b>a</b>) b = 2 μm; (<b>b</b>) b = 5 μm; (<b>c</b>) b = 7.5 μm; (<b>d</b>) b = 10 μm.</p>
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13 pages, 4685 KiB  
Article
High-Performance SAW-Based Microfluidic Actuators Composed of Sputtered Al–Cu IDT Electrodes
by Hwansun Kim, Youngjin Lee, Peddathimula Puneetha, Sung Jin An, Jae-Cheol Park and Siva Pratap Reddy Mallem
Coatings 2024, 14(11), 1420; https://doi.org/10.3390/coatings14111420 - 8 Nov 2024
Viewed by 453
Abstract
To realize highly sensitive SAW devices, novel Al–Cu thin films were developed using a combinatorial sputtering system. The Al–Cu sample library exhibited a wide range of chemical compositions and electrical resistivities, providing valuable insights for selecting optimal materials for SAW devices. Considering the [...] Read more.
To realize highly sensitive SAW devices, novel Al–Cu thin films were developed using a combinatorial sputtering system. The Al–Cu sample library exhibited a wide range of chemical compositions and electrical resistivities, providing valuable insights for selecting optimal materials for SAW devices. Considering the significant influence of electrode resistivity and density on acoustic wave propagation, an Al–Cu film with 65 at% Al was selected as the IDT electrode material. The selected Al–Cu film demonstrated a resistivity of 6.0 × 10−5 Ω-cm and a density of 4.4 g/cm3, making it suitable for SAW-based microfluidic actuator applications. XRD analysis revealed that the Al–Cu film consisted of a physical mixture of Al and Cu without the formation of Al–Cu alloy phases. The film exhibited a fine-grained microstructure with an average crystallite size of 7.5 nm and surface roughness of approximately 6 nm. The SAW device fabricated with Al–Cu IDT electrodes exhibited excellent acoustic performance, resonating at 143 MHz without frequency shift and achieving an insertion loss of −13.68 dB and a FWHM of 0.41 dB. In contrast, the Au electrode-based SAW device showed significantly degraded acoustic characteristics. Moreover, the SAW-based microfluidic module equipped with optimized Al–Cu IDT electrodes successfully separated 5 μm polystyrene (PS) particles even at high flow rates, outperforming devices with Au IDT electrodes. This enhanced performance can be attributed to the improved resonance characteristics of the SAW device, which resulted in a stronger acoustic radiation force exerted on the PS particles. Full article
(This article belongs to the Special Issue Thin Films and Nanostructures for Electronics)
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<p>Schematic diagram of combinatorial sputtering to produce Al–Cu thin films with varying and uniform compositions.</p>
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<p>Thickness distribution and cross-section images of Al–Cu thin films [<a href="#B25-coatings-14-01420" class="html-bibr">25</a>].</p>
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<p>Surface and cross-sectional SEM images of Al–Cu thin films with uniform thickness and compositions.</p>
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<p>XRD patterns of Al–Cu thin films with uniform physical and chemical properties.</p>
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<p>AFM topography images of sputter-deposited Al–Cu thin films (S1, S2, S3) with different surface roughness values.</p>
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<p>SAW-IDT pattern design for separating 5 μm PS micro-particles. (<b>a</b>) Distribution of resonant frequency depending on IDT pattern width and (<b>b</b>) relationship between total IDT length and electrode pairs at the reference impedance of 50 Ω.</p>
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<p>Resonant frequency of SAW devices with Al–Cu and Au electrode.</p>
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<p>SAW-based microfluidic actuator module for 5 μm PS particle separation. (<b>a</b>) Picture of SAW-based microfluidic actuator module and (<b>b</b>) separation efficiency of PS particles according to the flow rate of PS suspension with a concentration of 100 μg/L.</p>
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<p>Optical microscope images of PS particles captured at the drain/outlet ports in the SAW actuator module consisting of two different electrodes.</p>
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13 pages, 7956 KiB  
Article
Design and Investigation of a High-Performance Quartz-Based SAW Temperature Sensor
by Jianfei Jiang
Micromachines 2024, 15(11), 1349; https://doi.org/10.3390/mi15111349 - 31 Oct 2024
Viewed by 614
Abstract
In this work, a surface acoustic wave (SAW) temperature sensor based on a quartz substrate was designed and investigated. Employing the Coupling-of-Modes (COM) model, a detailed analysis was conducted on the effects of the number of interdigital transducers (IDTs), the number of reflectors, [...] Read more.
In this work, a surface acoustic wave (SAW) temperature sensor based on a quartz substrate was designed and investigated. Employing the Coupling-of-Modes (COM) model, a detailed analysis was conducted on the effects of the number of interdigital transducers (IDTs), the number of reflectors, and their spacing on the performance of the SAW device. The impact of the transversal mode of quartz SAWs on the device was subsequently examined using the finite element method (FEM). The simulation results indicate that optimizing these structural parameters significantly enhances the sensor’s sensitivity and frequency stability. SAW devices with optimal structural parameters were fabricated, and their resonant frequencies were tested across a temperature range of 25–150 °C. Experimental results demonstrate that the SAW temperature sensor maintains high performance stability and data reliability throughout the entire temperature range, achieving a Bode-Q of 7700. Furthermore, the sensor exhibits excellent linearity and repeatability. An analysis of the sensor’s response under varying temperature conditions reveals a significant temperature dependency on its Temperature Coefficient of Frequency (TCF). This feature suggests that the sensor possesses potential advantages for applications in industrial process control and environmental monitoring. Full article
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<p>(<b>a</b>) Schematic diagram of the 2D periodic model of the SAW device; (<b>b</b>) mode shapes of the symmetric and antisymmetric modes of the Rayleigh wave; (<b>c</b>) top view of the 3D periodic model of the SAW device.</p>
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<p>Top view of the complete SAW resonator structure.</p>
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<p>Simulation results for SAW resonators with different NI: (<b>a</b>) impedance curves, (<b>b</b>) Bode-Q curves, and (<b>c</b>) Bode-Q values (top) and impedance variation values (bottom) at the resonance point; for SAW resonators with different NR: (<b>d</b>) impedance curves, (<b>e</b>) Bode-Q curves, and (<b>f</b>) Bode-Q values (top) and impedance variation values (bottom) at the resonance point.</p>
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<p>Simulated impedance curves corresponding to <b><span class="html-italic">L</span></b><sub>g</sub> for (<b>a</b>) λ/8 + nλ/2 (n = 0, 1, 2) and (<b>b</b>) λ/4 + nλ/8 (n = 0, 1, 2, 3).</p>
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<p>(<b>a</b>) Admittance curve of the SAW without the dummy structure; (<b>b</b>) admittance and conductance curves of the SAW device with different dummy length designs.</p>
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<p>(<b>a</b>) Simulated reflection coefficient curves of the device at different temperatures; (<b>b</b>) resonant frequency and minimum reflection coefficient of the sensor at different temperatures.</p>
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<p>SEM image of the SAW resonator with a wavelength of 7.2 μm.</p>
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<p>Test setup and procedure for temperature sensor evaluation.</p>
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<p>(<b>a</b>) Impedance curve and S11 test results of the SAW device at 30 °C; (<b>b</b>) Bode-Q curve of the device at 30 °C; and (<b>c</b>) variation of the sensor’s resonant frequency at different temperatures. (<b>d</b>) Error chart of temperature sensor tested multiple times.</p>
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12 pages, 2930 KiB  
Article
Ultrasonic A-Scan Signals Data Augmentation Using Electromechanical System Modelling to Enhance Cataract Classification Methods
by Mário J. Santos, Lorena I. Petrella, Fernando Perdigão and Jaime Santos
Electronics 2024, 13(21), 4144; https://doi.org/10.3390/electronics13214144 - 22 Oct 2024
Viewed by 554
Abstract
The use of artificial intelligence in diverse diagnosis areas has significantly increased in the past few years because of the advantages it represents in clinical routine. Among the diverse diagnostic techniques, the use of ultrasounds is often preferred because of their simplicity, low [...] Read more.
The use of artificial intelligence in diverse diagnosis areas has significantly increased in the past few years because of the advantages it represents in clinical routine. Among the diverse diagnostic techniques, the use of ultrasounds is often preferred because of their simplicity, low cost, non-invasiveness, and non-ionizing characteristic. However, obtaining an adequate number of patients and data for training and testing machine learning models is challenging. To overcome this limitation, a novel approach is proposed for simulating data produced by ultrasonic diagnostic devices. The implemented method was based on a clinical prototype for eye cataract diagnosis, although the method can be extended to other applications as well. The proposed model encompasses the electric-to-acoustic signal conversion in the ultrasonic transducer, the wave propagation through the biological medium, and the subsequent acoustic-to-electric signal conversion in the transducer. Electrical modelling of the transducer was performed using a two-port network approach, while the acoustic wave propagation was modelled by using the k-Wave MATLAB toolbox. It was verified that the holistic modelling approach enabled the generation of synthetic data augmentation, presenting high similarity with real data. Full article
(This article belongs to the Special Issue Feature Papers in Circuit and Signal Processing)
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<p>Computational grids: 2D (<b>a</b>) and 3D (<b>b</b>). Components: cornea surface (yellow), cornea (green), aqueous humor (light blue), lens (purple), and vitreous humor (red). Outer limits of the eye in 2D grid (black and light grey).</p>
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<p>Electric circuit models for the pulse-echo system. (<b>a</b>) Emitter stage (<span class="html-italic">F</span> = 0); (<b>b</b>) Receiver stage (<span class="html-italic">V<sub>in</sub></span> = 0); (<b>c</b>,<b>d</b>) Simplification of the equivalent circuits to the primary side of the transformer for the emitter and the receiver stages, respectively. <span class="html-italic">V<sub>in</sub></span> is the excitation voltage source and <span class="html-italic">Z<sub>i</sub></span> its output impedance; <span class="html-italic">Z<sub>E</sub></span> and <span class="html-italic">Z<sub>m</sub></span> are the electric and mechanical impedances of the transducer; <span class="html-italic">ϕ</span> is equivalent to a transform ratio; <span class="html-italic">V</span><sub>1</sub> and <span class="html-italic">I</span><sub>1</sub> are the voltage and the current on the electrical side; <span class="html-italic">F</span><sub>1</sub> and <span class="html-italic">U</span><sub>1</sub> are the force and transducer surface velocity on the acoustic side; <span class="html-italic">Z<sub>L</sub></span> is the low-noise amplifier (LNA) input impedance.</p>
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<p>Signals used to validate the implemented model: (<b>a</b>) Electrical excitation signal <span class="html-italic">v</span><sub>1</sub>(<span class="html-italic">t</span>); (<b>b</b>) Simulated echo signal <span class="html-italic">p</span><sub>2</sub>(<span class="html-italic">t</span>) reflected in a flat metal plate; (<b>c</b>) Electrical echo signal from the reflector <span class="html-italic">v</span><sub>2</sub>(<span class="html-italic">t</span>); (<b>d</b>) Experimental and estimated received signals according to Equation (7).</p>
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<p>Signals used to validate the implemented model: (<b>a</b>) Electrical excitation signal <span class="html-italic">v</span><sub>1</sub>(<span class="html-italic">t</span>); (<b>b</b>) Simulated echo signal <span class="html-italic">p</span><sub>2</sub>(<span class="html-italic">t</span>) reflected in a flat metal plate; (<b>c</b>) Electrical echo signal from the reflector <span class="html-italic">v</span><sub>2</sub>(<span class="html-italic">t</span>); (<b>d</b>) Experimental and estimated received signals according to Equation (7).</p>
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<p>Transfer functions obtained when a flat reflector is placed at the focus of the transducer: (<b>a</b>) <span class="html-italic">H</span>(<span class="html-italic">s</span>); (<b>b</b>) <span class="html-italic">H</span><sub>2</sub>(<span class="html-italic">s</span>).</p>
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<p>Impulse response <span class="html-italic">h</span><sub>2</sub>(<span class="html-italic">t</span>) as the inverse Fourier transform of <span class="html-italic">H</span><sub>2</sub>(<span class="html-italic">jω</span>) shown in <a href="#electronics-13-04144-f004" class="html-fig">Figure 4</a>b.</p>
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<p>(<b>a</b>) Real signal from a healthy lens, <span class="html-italic">v</span><sub>2</sub>(<span class="html-italic">t</span>). (<b>b</b>) Estimated signal from a healthy lens, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>v</mi> <mo>^</mo> </mover> <mn>2</mn> </msub> <mfenced> <mi>t</mi> </mfenced> </mrow> </semantics></math>. The figures also show the pulse square integration with a window of 1 μs (red line) and points corresponding to 10% and 90% of the rise time (circles in red and blue, respectively).</p>
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<p>Estimated signal <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>v</mi> <mo>^</mo> </mover> <mn>2</mn> </msub> <mfenced> <mi>t</mi> </mfenced> </mrow> </semantics></math> from a cataractous lens.</p>
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14 pages, 6575 KiB  
Article
Enhanced Acoustic Mixing in Silicon-Based Chips with Sharp-Edged Micro-Structures
by Mehrnaz Hashemiesfahan, Pierre Gelin, Han Gardeniers and Wim De Malsche
Micro 2024, 4(4), 585-598; https://doi.org/10.3390/micro4040036 - 20 Oct 2024
Viewed by 690
Abstract
The small dimensions of microfluidic channels allow for fast diffusive or passive mixing, which is beneficial for time-sensitive applications such as chemical reactions, biological assays, and the transport of to-be-detected species to sensors. In microfluidics, the need for fast mixing within milliseconds arises [...] Read more.
The small dimensions of microfluidic channels allow for fast diffusive or passive mixing, which is beneficial for time-sensitive applications such as chemical reactions, biological assays, and the transport of to-be-detected species to sensors. In microfluidics, the need for fast mixing within milliseconds arises primarily because these devices are often used in fields where rapid and efficient mixing significantly impacts the performance and outcome of the processes. Active mixing with acoustics in microfluidic devices involves using acoustic waves to enhance the mixing of fluids within microchannels. Using sharp corners and wall patterns in acoustofluidic devices significantly enhances the mixing by acoustic streaming around these features. The streaming patterns around the sharp edges are particularly effective for the mixing because they can produce strong lateral flows that rapidly homogenize liquids. This work presents extensive characterizations of the effect of sharp-edged structures on acoustic mixing in bulk acoustic wave (BAW) mode in a silicon microdevice. The effect of side wall patterns in different angles and shapes, their positions, the type of piezoelectric transducer, and its amplitude and frequency have been studied. Following the patterning of the channel walls, a mixing time of 25 times faster was reached, compared to channels with smooth side walls exhibiting conventional BAW behavior. The average locally determined acoustic streaming velocity inside the channel becomes 14 times faster if sharp corners of 10° are added to the wall. Full article
(This article belongs to the Section Analysis Methods and Instruments)
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<p>(<b>a</b>) The acoustofluidic setup schematic, including the microchip and PZT transducer, is fixed in a PMMA holder. (<b>b</b>) The schematics of the different device designs used: (device a) Microdevice with periodic 30° sharp edge; (device b) Microdevice with 10°, 20°, 30°, 40°, 50°, and 60°sharp edge; (device c) Microdevice with sharp corners with various tip shapes; (device d) Microdevice with triangular pillars in the middle of the channel; (device e) Microdevice with circular pillars amid the channel.</p>
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<p>A SEM image of the sharp corners etched alongside the silicon microfluidic channel in device a.</p>
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<p>The resulting streaming velocity for a range of PZT devices and applied frequencies. The experiments for each condition were repeated three times, and the movies were recorded. For each movie, a random number between 15 and 25 particles was tracked, and the average streaming velocity was indicated. The error bars are twice the standard deviation of the three average streaming velocities.</p>
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<p>The mixing efficiency experiments and a graph representing the results. The top image shows a continuous flow of water in the middle and fluorescent dye from both sides when the acoustics are off. The bottom image is when the acoustics have turned on, and the water and fluorescent dye are mixed. The graph extracted from MATLAB shows that the mixing efficiency reached almost 80% in 0.2 s.</p>
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<p>The velocity vectors (arrows in red) of the acoustic streaming around the sharp edges on the side wall of the silicon channel (device a) when 7 V (<b>left</b>) and 20 V (<b>right</b>) voltage are applied. Please refer to <a href="#app1-micro-04-00036" class="html-app">SI (SI)</a>, <a href="#app1-micro-04-00036" class="html-app">S1</a> (7 V), and <a href="#app1-micro-04-00036" class="html-app">S2</a> (20 V) for the recorded <a href="#app1-micro-04-00036" class="html-app">experimental video</a>.</p>
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<p>The effect of different angles of sharp corners (device b) on the average velocity magnitude. The images are taken from the chip from the top with an optical microscope. The channels with 10°, 20°, and (30°, 40°, and 60°) result in 14, 8, and 1.5 times faster streaming consecutively compared to a straight channel with the same width and depth at 28 V.</p>
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<p>(<b>a</b>–<b>d</b>) The z-stacking of 1 µm polystyrene particles movement along the acoustic streaming around the sharp corners with numerous tip shapes. The tip shapes shown in green are the initially designed tip and the above image of them is taken with an optical microscope after the device has been fabricated.</p>
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<p>A column graph of the effect of sharp tip and analyzed area on the average velocity magnitude. The blue bars are the measured average velocity in a 2.5 times bigger area (blue dashed lines) and measured average velocity in the smaller area (dashed green lines) are depicted as green bars.</p>
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<p>The z-stacking of the particle movements in the channel of device d with triangular pillars. The top-left image shows all the frames since the start of streaming and pumping on top of one another.</p>
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<p>(<b>a</b>) The z-stacking of particle movements in the channel of device e with circular pillars. The top-left image is all the frames since the start of streaming and pumping on top of each other. (<b>b</b>) A cross-section of an etched feature showing the scallop formation that causes circulation in the circular pillars (number 1 in the figure is 0.80 µm and number 2 is 3.33 µm).</p>
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<p>(<b>a</b>) Before the pumping starts, liquid movement patterns form inside the channel around each pillar, which increases with an increase in amplitude. The flow velocity in the channel with triangular pillars is higher than that with circular pillars. (<b>b</b>) After the pumping effect starts, the pumping velocity increases with time. This increase is more significant in the channel with triangular pillars.</p>
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18 pages, 5782 KiB  
Article
Quasi-Optical Four-Port Acoustic Filters Based on NEMS Coupled Beam Arrays
by Richard Syms
Micromachines 2024, 15(10), 1257; https://doi.org/10.3390/mi15101257 - 14 Oct 2024
Viewed by 663
Abstract
Theoretical models are presented for quasi-optical four-port acoustic devices based on NEMS-coupled beam arrays. Analogies with coupled mode devices in microwaves, ultrasonics, optics, and electron wave optics are first reviewed, together with coupled beam filters. Power transfer between two mechanically coupled, electrostatically driven, [...] Read more.
Theoretical models are presented for quasi-optical four-port acoustic devices based on NEMS-coupled beam arrays. Analogies with coupled mode devices in microwaves, ultrasonics, optics, and electron wave optics are first reviewed, together with coupled beam filters. Power transfer between two mechanically coupled, electrostatically driven, coupled beam arrays is then demonstrated using a lumped element model, and the conditions for full power transfer are established. Four-port devices, including directional couplers and coupler filters with complementary transmission ports, are then demonstrated. Predictions are verified for realistic device layouts using the stiffness matrix method. Full article
(This article belongs to the Special Issue The 15th Anniversary of Micromachines)
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<p>Optical directional coupler: (<b>a</b>) layout and (<b>b</b>) switch response.</p>
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<p>Directional coupler filter: (<b>a</b>) layout; (<b>b</b>) dispersion characteristic (upper) and spectral variation of drop-port transmission (lower) [<a href="#B52-micromachines-15-01257" class="html-bibr">52</a>].</p>
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<p>Coupled beam filter: (<b>a</b>) layout; (<b>b</b>) full and (<b>c</b>) reduced lumped element models.</p>
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<p>(<b>a</b>) Response of coupled beam filter; (<b>b</b>) dispersion characteristic of coupled beam array.</p>
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<p>Acoustic directional coupler: (<b>a</b>) layout and (<b>b</b>) lumped element model.</p>
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<p>Acoustic directional coupler: (<b>a</b>) dispersion characteristics and (<b>b</b>) variation of transmitted powers with number of beams.</p>
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<p>LEM model of acoustic directional coupler: frequency dependence of S-parameters for (<b>a</b>) transmission and (<b>b</b>) reflection ports.</p>
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<p>Acoustic coupler filter: (<b>a</b>) layout and (<b>b</b>) lumped element model.</p>
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<p>LEM model of acoustic coupler filter: (<b>a</b>) dispersion characteristics, (<b>b</b>) frequency dependence of S-parameters.</p>
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<p>SMM model of acoustic coupler: (<b>a</b>) complete layout and (<b>b</b>) enlarged partial view.</p>
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<p>SMM model of acoustic directional coupler: (<b>a</b>) dispersion characteristics and (<b>b</b>) variation in transmitted powers with number of beams.</p>
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<p>SMM model of acoustic directional coupler: frequency dependence of S-parameters for (<b>a</b>) transmission and (<b>b</b>) reflection ports.</p>
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<p>SMM model of acoustic coupler filter: (<b>a</b>) layout and (<b>b</b>) enlarged partial view after tuning.</p>
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<p>SMM model of acoustic coupler filter: frequency dependence of S-parameters for (<b>a</b>) transmission and (<b>b</b>) reflection ports.</p>
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12 pages, 5227 KiB  
Article
Honeycomb-Shaped Phononic Crystals on 42°Y-X LiTaO3/SiO2/Poly-Si/Si Substrate for Improved Performance and Miniaturization
by Panliang Tang, Hongzhi Pan, Temesgen Bailie Workie, Jia Mi, Jingfu Bao and Ken-ya Hashimoto
Micromachines 2024, 15(10), 1256; https://doi.org/10.3390/mi15101256 - 14 Oct 2024
Viewed by 2242
Abstract
A SAW device with a multi-layered piezoelectric substrate has excellent performance due to its high Q value. A multi-layer piezoelectric substrate combined with phononic crystal structures capable of acoustic wave reflection with a very small array can achieve miniaturization and high performance. In [...] Read more.
A SAW device with a multi-layered piezoelectric substrate has excellent performance due to its high Q value. A multi-layer piezoelectric substrate combined with phononic crystal structures capable of acoustic wave reflection with a very small array can achieve miniaturization and high performance. In this paper, a honeycomb-shaped phononic crystal structure based on 42°Y-X LT/SiO2/poly-Si/Si-layered substrate is proposed. The analysis of the bandgap distribution under various filling fractions was carried out using dispersion and transmission characteristics. In order to study the application of PnCs in SAW devices, one-port resonators with different reflectors were compared and analyzed. Based on the frequency response curves and Bode-Q value curves, it was found that when the HC-PnC structure is used as a reflector, it can not only improve the transmission loss of the resonator but also reduce the size of the device. Full article
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<p>Top view of HC-PnC unit cell with its IBZ.</p>
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<p>Three-dimensional view of the HC-PnC unit cell.</p>
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<p>(<b>a</b>) Schematic 3D representation of the proposed PnC; (<b>b</b>) schematic representation of a transmission line composed of an array of 5 unit cells of the proposed PnC.</p>
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<p>(<b>a</b>) Dispersion curve of acoustic waves for the HC-PnC; (<b>b</b>) simulated transmission curve through a finite strip.</p>
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<p>Dispersion curve and simulated transmission curve with different filling fractions. (<b>a</b>) dispersion curve with <span class="html-italic">p</span> = 1.4 μm. (<b>b</b>) simulated transmission curve with <span class="html-italic">p</span> = 1.4 μm. (<b>c</b>) dispersion curve with <span class="html-italic">p</span> = 1.6 μm. (<b>d</b>) simulated transmission curve with p = 1.6 μm. (<b>e</b>) dispersion curve with <span class="html-italic">p</span> = 2.0 μm. (<b>f</b>) simulated transmission curve with <span class="html-italic">p</span> = 2.0 μm. (<b>g</b>) dispersion curve with <span class="html-italic">p</span> = 2.2 μm. (<b>h</b>) simulated transmission curve with <span class="html-italic">p</span> = 2.2 μm.</p>
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<p>Dispersion curve and simulated transmission curve with different filling fractions. (<b>a</b>) dispersion curve with <span class="html-italic">p</span> = 1.4 μm. (<b>b</b>) simulated transmission curve with <span class="html-italic">p</span> = 1.4 μm. (<b>c</b>) dispersion curve with <span class="html-italic">p</span> = 1.6 μm. (<b>d</b>) simulated transmission curve with p = 1.6 μm. (<b>e</b>) dispersion curve with <span class="html-italic">p</span> = 2.0 μm. (<b>f</b>) simulated transmission curve with <span class="html-italic">p</span> = 2.0 μm. (<b>g</b>) dispersion curve with <span class="html-italic">p</span> = 2.2 μm. (<b>h</b>) simulated transmission curve with <span class="html-italic">p</span> = 2.2 μm.</p>
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<p>A schematic 3D representation of a one-port SAW resonator with (<b>a</b>) 3 HC-PnCs as a reflector and (<b>b</b>) 3 pairs of reflective gratings.</p>
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<p>(<b>a</b>) Simulated admittance (Y) response and (<b>b</b>) simulated Bode-Q of a one-port SAW resonator with 3HC-PnCs as a reflector vs. 3 pairs of reflective gratings.</p>
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<p>A one-port SAW resonator 3D model with an incomplete etched LT layer and the detailed model.</p>
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<p>(<b>a</b>) Simulated frequency response curve and (<b>b</b>) simulated transmission curve with different PnC thicknesses.</p>
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13 pages, 2694 KiB  
Article
Tracking the Risk of Cardiovascular Disease after Almond and Oat Milk Intervene or Statin Medication with a Powerful Reflex SH-SAW POCT Platform
by Chia-Hsuan Cheng, Hiromi Yatsuda, Han-Hsiang Chen, Guang-Huar Young, Szu-Heng Liu and Robert YL Wang
Sensors 2024, 24(20), 6517; https://doi.org/10.3390/s24206517 - 10 Oct 2024
Viewed by 656
Abstract
Cardiovascular disease (CVD) represents the leading cause of death worldwide. For individuals at elevated risk for cardiovascular disease, early detection and monitoring of lipid status is imperative. The majority of lipid measurements conducted in hospital settings employ optical detection, which necessitates the use [...] Read more.
Cardiovascular disease (CVD) represents the leading cause of death worldwide. For individuals at elevated risk for cardiovascular disease, early detection and monitoring of lipid status is imperative. The majority of lipid measurements conducted in hospital settings employ optical detection, which necessitates the use of relatively large-sized detection machines. It is, therefore, necessary to develop point-of-care testing (POCT) for lipoprotein in order to monitor CVD. To enhance the management and surveillance of CVD, this study sought to develop a POCT approach for apolipoprotein B (ApoB) utilizing a shear horizontal surface acoustic wave (SH-SAW) platform to assess the risk of heart disease. The platform employs a reflective SH-SAW sensor to reduce the sensor size and enhance the phase-shifted signals. In this study, the platform was utilized to monitor the impact of a weekly almond and oat milk or statins intervention on alterations in CVD risk. The SH-SAW ApoB test exhibited a linear range of 0 to 212 mg/dL, and a coefficient correlation (R) of 0.9912. Following a four-week intervention period, both the almond and oat milk intervention (−23.3%, p < 0.05) and statin treatment (−53.1%, p < 0.01) were observed to significantly reduce ApoB levels. These findings suggest that the SH-SAW POCT device may prove a valuable tool for monitoring CVD risk, particularly during routine daily or weekly follow-up visits. Full article
(This article belongs to the Section Biosensors)
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<p>The reflective SH-SAW biosensor chip employs a measurement system and structure comprising a forked finger sensor (IDT), a gold sensing area, and a reflector.</p>
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<p>Operation of the iProtin reader with ApoB SH-SAW biosensor.</p>
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<p>Recruitment and categorization of participants.</p>
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<p>Schedule for measuring cardiovascular indices.</p>
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<p>Establishment of 4PL fitting curve. (<b>a</b>) The real time curves of various ApoB concentrations. The darker line represents a higher concentration, the red lines indicate the slope at 10–30 s, which were used to establish the 4PL fitting curve; (<b>b</b>) 4PL fitting curve of ApoB chips based on the 10–30 s slope of the real-time curve.</p>
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<p>The comparison study of the SH-SAW biosensor and the commercially available product.</p>
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<p>Follow-up of ApoB concentration after 12 weeks of food therapy intervention.</p>
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<p>The change of ApoB concentrations at 4, 8, and 12 weeks after the food therapy.</p>
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<p>Comparison of ApoB-lowering effects in the food therapy group versus the statin treatment group: (<b>a</b>) line chart; (<b>b</b>) box plot.</p>
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<p>Comparison of the effect of food therapy group in reducing the high-ApoB-baseline (&gt;100 mg/dL) and the low-ApoB-baseline (&lt;100 mg/dL) groups: (<b>a</b>) line chart; (<b>b</b>) box plot.</p>
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24 pages, 5693 KiB  
Review
Physical Sensors Based on Lamb Wave Resonators
by Zixia Yu, Yongqing Yue, Zhaozhao Liang, Xiaolong Zhao, Fangpei Li, Wenbo Peng, Quanzhe Zhu and Yongning He
Micromachines 2024, 15(10), 1243; https://doi.org/10.3390/mi15101243 - 9 Oct 2024
Viewed by 2935
Abstract
A Lamb wave is a guided wave that propagates within plate-like structures, with its vibration mode resulting from the coupling of a longitudinal wave and a shear vertical wave, which can be applied in sensors, filters, and frequency control devices. The working principle [...] Read more.
A Lamb wave is a guided wave that propagates within plate-like structures, with its vibration mode resulting from the coupling of a longitudinal wave and a shear vertical wave, which can be applied in sensors, filters, and frequency control devices. The working principle of Lamb wave sensors relies on the excitation and propagation of this guided wave within piezoelectric material. Lamb wave sensors exhibit significant advantages in various sensing applications due to their unique wave characteristics and design flexibility. Compared to traditional surface acoustic wave (SAW) and bulk acoustic wave (BAW) sensors, Lamb wave sensors can not only achieve higher frequencies and quality factors in smaller dimensions but also exhibit superior integration and multifunctionality. In this paper, we briefly introduce Lamb wave sensors, summarizing methods for enhancing their sensitivity through optimizing electrode configurations and adjusting piezoelectric thin plate structures. Furthermore, this paper systematically explores the development of Lamb wave sensors in various sensing applications and provides new insights into their future development. Full article
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<p>Classification of applications and detection parameters for LWRs as sensors.</p>
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<p>Two topologies of LWRs: (<b>a</b>) edge-type and (<b>b</b>) grating-type.</p>
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<p>Four transducer configurations of single-port LWRs [<a href="#B36-micromachines-15-01243" class="html-bibr">36</a>]: (<b>a</b>) single-IDT; (<b>b</b>) IDT/grounded-BE; (<b>c</b>) IDT/floating-BE; (<b>d</b>) double-IDT.</p>
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<p>Effective electromechanical coupling coefficient of four transducer configurations in AlN thin plates of S<sub>0</sub> mode [<a href="#B36-micromachines-15-01243" class="html-bibr">36</a>], where <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>p</mi> </msub> </mrow> </semantics></math> is the parallel resonant frequency and <math display="inline"><semantics> <mrow> <msub> <mi>f</mi> <mi>s</mi> </msub> </mrow> </semantics></math> is the series resonant frequency. The thickness of the piezoelectric thin plate affects the resonant frequency, which, in turn, influences the <math display="inline"><semantics> <mrow> <msubsup> <mi>k</mi> <mrow> <mi>e</mi> <mi>f</mi> <mi>f</mi> </mrow> <mn>2</mn> </msubsup> </mrow> </semantics></math>. Different colored lines represent different transducers, and their structures are shown in the figure.</p>
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<p>(<b>a</b>) Two modes of the Lamb wave; (<b>b</b>) schematic diagram of a finite-length thin plate.</p>
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<p>Comparison of acoustic impedance, Young’s modulus, and density for different electrode materials [<a href="#B88-micromachines-15-01243" class="html-bibr">88</a>]. All parameter values are normalized relative to the characteristics of AlN.</p>
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<p>Common LWR biosensors [<a href="#B12-micromachines-15-01243" class="html-bibr">12</a>]: (<b>a</b>) structural design; (<b>b</b>) cross-sectional diagram.</p>
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<p>Applications of LWR biosensors: (<b>a</b>) electrode structure and model diagram of an inverted LWR biosensor based on ZnO/SiO<sub>2</sub>/Si/ZnO film [<a href="#B13-micromachines-15-01243" class="html-bibr">13</a>]; (<b>b</b>) schematic diagram of a flexible acoustic sensor for biosensing based on LFE-TSM/Lamb wave hybrid mode [<a href="#B14-micromachines-15-01243" class="html-bibr">14</a>].</p>
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<p>Curves showing the influence of piezoelectric film thickness on sensor sensitivity [<a href="#B12-micromachines-15-01243" class="html-bibr">12</a>].</p>
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<p>Four coupling configurations of LWR liquid sensors [<a href="#B100-micromachines-15-01243" class="html-bibr">100</a>]: (<b>a</b>) sfT; (<b>b</b>) smfT; (<b>c</b>) sTf; (<b>d</b>) sTfm.</p>
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<p>Curves of effective electromechanical coupling coefficients for four coupling configurations on c-AlN/SiC (001) &lt;100&gt; substrates [<a href="#B100-micromachines-15-01243" class="html-bibr">100</a>]: (<b>a</b>) sfT; (<b>b</b>) smfT; (<b>c</b>) sTf; (<b>d</b>) sTfm.</p>
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<p>Applications of LWR liquid sensors: (<b>a</b>) model and physical diagram of a density and viscosity decoupled AlN Lamb wave sensor [<a href="#B16-micromachines-15-01243" class="html-bibr">16</a>]; (<b>b</b>) two-dimensional array model broken view of a Lamb wave viscosity sensor [<a href="#B15-micromachines-15-01243" class="html-bibr">15</a>].</p>
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<p>Applications of LWR pressure sensors: (<b>a</b>) lateral field excited (LFE) Lamb wave resonator for high-temperature pressure sensing [<a href="#B46-micromachines-15-01243" class="html-bibr">46</a>]; (<b>b</b>) structural diagram of a piezoelectric sensor based on dual modes (LFE Lamb wave mode and SAW mode) [<a href="#B22-micromachines-15-01243" class="html-bibr">22</a>]; (<b>c</b>) 3D structure diagram and cross-sectional of the dual-temperature-compensated Lamb wave pressure sensor [<a href="#B23-micromachines-15-01243" class="html-bibr">23</a>].</p>
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<p>Structural and physical diagram of a flexible dual-mode (A<sub>0</sub> and S<sub>0</sub>) LWR humidity sensor [<a href="#B19-micromachines-15-01243" class="html-bibr">19</a>].</p>
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