Transducer sample and performance test. (a) The fabricated matching layer has a diameter of 20 mm and a thickness of 1000 μ m. A transducer was fabricated to demonstrate the performance and practical use of this new metamaterial matching layer. A low acoustic impedance porous piezoelectric ceramic slab with a centre frequency of 4 MHz was used in this transducer. The acoustic impedance of the backing material is 7.8 MRayls. (b) The pulse echo tests were conducted on a 1 cm thick polystyrene test block. An aluminium plate acted as the acoustic total reflection body. The traditional λ /4 acoustic impedance matching layer transducer was tested using the same equipment for comparison.  

Transducer sample and performance test. (a) The fabricated matching layer has a diameter of 20 mm and a thickness of 1000 μ m. A transducer was fabricated to demonstrate the performance and practical use of this new metamaterial matching layer. A low acoustic impedance porous piezoelectric ceramic slab with a centre frequency of 4 MHz was used in this transducer. The acoustic impedance of the backing material is 7.8 MRayls. (b) The pulse echo tests were conducted on a 1 cm thick polystyrene test block. An aluminium plate acted as the acoustic total reflection body. The traditional λ /4 acoustic impedance matching layer transducer was tested using the same equipment for comparison.  

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High-quality broadband ultrasound transducers yield superior imaging performance in biomedical ultrasonography. However, proper design to perfectly bridge the energy between the active piezoelectric material and the target medium over the operating spectrum is still lacking. Here, we demonstrate a new anisotropic cone-structured acoustic metamateri...

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... [6][7][8] To overcome the problem of narrowband, composite structures stacking two or more quarterwavelength layers have been extensively studied to achieve broadband sound transmission, [9][10][11][12][13][14][15] in which a challenging work is to obtain suitable matching layers with specific impedance. In comparison, some acoustic metamaterials with deep sub-wavelength structure, 5,16,17 periodic phononic crystal, 18 and gradient refractive index material [19][20][21] have been implemented to break through the limitations in material availability and achieve broadband acoustic impedance matching. ...
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... There have been many studies on acoustic metamaterials over the last decade [2][3][4][5][6][7][8][9][10][11]. Acoustic metamaterials are structures in which fine structures are created within the material and behavior as if the acoustic properties of the material are controlled. ...
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... Looking at tunable acoustic metamaterials suitable for sound reduction, most of the approaches seem to be combine piezo with acoustic metamaterials [109][110][111][112]. A theoretical examination of an acoustic metamaterials consisting of piezoelectric boundaries was carried out [113]. ...
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... This mismatch results in reduced transmission efficiency. Li et al. [13] developed an acoustic metamaterial matching layer with an anisotropy conical structure, which has an acoustic impedance gradient from 11.4 to 3.0 MRayls in the direction of its thickness, effectively transiting the acoustic impedance difference between the piezoelectric material and the target medium, allowing the transducer to transmit ultrasonic waves over a wide frequency range. This design has a great improvement compared with the traditional design, and provides a practical solution for the impedance matching of medical ultrasonic transducer. ...
... In addition, during the development and testing of acoustic metamaterials, a frequencyresolved broadband characterisation of materials is necessary. Examples of metamaterials with dispersive longitudinal waves can be found in the literature [10][11][12]. Thus, broadband, frequency-resolved measurements of sound velocity and attenuation open up new possibilities for materials analysis. ...
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... DLs are generally fabricated using a single material, and their impedance is matched only with the sensor, leading to a potentially large impedance mismatch between the target and DL. If the impedance mismatch is large, it causes a large amount of the acoustic energy to be reflected at the interface, and also creates a strong standing wave in the DL [7]. A single quarter wavelength matching (λ/4) layer is a popular solution to couple the source and target that has different impedance by taking advantage of the constructive and destructive interferences in the matching layer [8,9]. ...
... A single quarter wavelength matching (λ/4) layer is a popular solution to couple the source and target that has different impedance by taking advantage of the constructive and destructive interferences in the matching layer [8,9]. However, this method leads to a narrow operational frequency range [7]. Stacking multiple matching layers would theoretically improve the broadband characteristic of transmission, but it undesirably lengthens the coupling medium, especially for low-frequency (20-100 KHz) applications. ...
... The problem of acoustic impedance mismatch has also started to be addressed by various groups using acoustic metamaterials [17][18][19][20]. Research work by [7,21,22] showed that graded impedance matching metamaterials can improve broadband energy transmission in high frequency (1)(2)(3)(4)(5) applications. ...
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... The superior acoustic performance of phonon crystals provides a new solution idea for the optimized design of the ultrasonic transducer. 23,24 In 2017, Li et al. 25 proposed acoustic metamaterial matching layers for broadband gradient impedance matching of ultrasonic transducers. In 2019, Han et al. 26 designed a singlecell UHF acoustic signal acquisition model for rotating bodies based on acoustic metamaterials, realizing the local field enhancement effect of the model at different frequencies. ...
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... However, there is still a lack of proper design to bridge the energy generated by a piezoelectric actuator and the target elastic medium over the wide operating spectrum [15]. The design of such devices needs to be optimized in order to maximize the energy transfer efficiency [16]. Thus, Li et al. [16] developed an anisotropic cone-structured EMM layer for matching piezoelectric actuator and substrate for improvement of broadband ultrasound transducers. ...
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... On the other hand, acoustic impedance gradient matching techniques have gained attention. Compared to traditional quarter-wavelength single/multi-layer matching techniques, acoustic impedance gradient matching effectively broadens the transducer's operating bandwidth and improves sensitivity, enhancing overall performance [11][12][13]. Phononic crystal, with its characteristics such as bandgaps and defective state, offers control over the propagation of sound and elastic waves [14][15][16]. Ji et al. [17,18] designed a phononic crystal air-coupled ultrasonic transducer. ...
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... The acoustic impedance gradient material has been proved to exhibit the characteristics of high-frequency conduction, and the quasi-continuous acoustic impedance change can be realized in the range of material by selecting the type of filler and adjusting the filling proportion [26,27]. Therefore, using an artificial acoustic impedance gradient composite is a promising way to solve the above problem [27,28]. In recent years, many researchers have tried to apply impedance gradient composites to ultrasonic transducers with traditional piezoelectric ceramics. ...
... In 2016, Lu prepared a new anisotropic conical ultrasonic matching layer material by etching the stripped silica fiber bundle in a hydrofluoric acid solution. The corresponding −6 dB bandwidth of the ultrasonic transducer equipped with this matching layer can reach 107%, which strongly proves that the acoustic impedance gradient matching material is suitable for the broadband sound transmission ability of a single crystal 28 . However, the acoustic impedance of this structure can only change linearly along the thickness direction, and because the acoustic impedance gradient is realized by using the change in the geometric size of the high impedance filler in the matching layer, this structure is only suitable for the frequency band where the wavelength is much larger than the chassis size of high impedance filler of each unit [28]. ...
... The corresponding −6 dB bandwidth of the ultrasonic transducer equipped with this matching layer can reach 107%, which strongly proves that the acoustic impedance gradient matching material is suitable for the broadband sound transmission ability of a single crystal 28 . However, the acoustic impedance of this structure can only change linearly along the thickness direction, and because the acoustic impedance gradient is realized by using the change in the geometric size of the high impedance filler in the matching layer, this structure is only suitable for the frequency band where the wavelength is much larger than the chassis size of high impedance filler of each unit [28]. ...
Article
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High-performance broadband ultrasound transducers provide superior imaging quality in biomedical ultrasound imaging. However, a matching design that perfectly transmits the acoustic energy between the active piezoelectric element and the target medium over the operating spectrum is still lacking. In this work, an anisotropic gradient acoustic impedance composite material as the matching layer of an ultrasonic transducer was designed and fabricated; it is a non-uniform material with the continuous decline of acoustic impedance along the direction of ultrasonic propagation in a sub-wavelength range. This material provides a broadband window for ultrasonic propagation in a wide frequency range and achieves almost perfect sound energy transfer efficiency from the piezoelectric material to the target medium. Nano tungsten particles and epoxy resin were selected as filling and basic materials, respectively. Along the direction of ultrasonic propagation, the proportion of tungsten powder was carefully controlled to decrease gradually, following the natural exponential form in a very narrow thickness range. Using this new material as a matching layer with high-performance single crystals, the −6 dB bandwidth of the PMN-PT ultrasonic transducer could reach over 170%, and the insertion loss was only −20.3 dB. The transducer achieved a temporal signal close to a single wavelength, thus there is the potential to dramatically improve the resolution and imaging quality of the biomedical ultrasound imaging system.