ライフサイエンスコーパス: piezoelectric

1 urface also implies that it is intrinsically piezoelectric.

2 dary interaction between biased and unbiased piezoelectric.

3 nt symmetry requirements to be classified as piezoelectric.

4 obates, K1-xNaxNbO3, are promising lead-free piezoelectrics.

5 oupled to strain, making ferroelectrics good piezoelectrics.

6 face engineering by local polarization using piezoelectric(1-4), pyroelectric(5,6) and ferroelectric(

7 Detection relies on the electromagnetic piezoelectric acoustic sensor (EMPAS) platform.

8 and the ultra-high frequency electromagnetic piezoelectric acoustic sensor (EMPAS).

9 ying the anomalously large, room temperature piezoelectric activity of relaxor-PbTiO(3) type single c

10 iable air cavity is controlled by means of a piezoelectric actuator that supports and varies the heig

11 TBI (dTBI) device, a platform that employs a piezoelectric actuator to reproducibly deliver a force i

12 und plane, which is controlled by means of a piezoelectric actuator.

13 a by precise compression of the head using a piezoelectric actuator.

14 t 0.3 megapascals) and comparable to ceramic piezoelectric actuators (about 40 megapascals)-and strai

15 four wings driven by two alumina-reinforced piezoelectric actuators to increase aerodynamic efficien

16 egatively charged nitrogen vacancy center in piezoelectric aluminum nitride exhibits spin-triplet gro

17 his paper, a chip-scale device consisting of piezoelectric Aluminum Nitride ultrasonic transducers wa

18 t offers a unique combination of substantial piezoelectric and birefringent properties, yet its lack

19 linked to low temperature relaxations in the piezoelectric and dielectric properties.

20 wire strain sensors and even piezoresistive, piezoelectric and ferroelectric nanodevices(14).

21 ontroversies regarding the dependence of the piezoelectric and ferroelectric properties on the grain

22 The first order gradiometer based on piezoelectric and magnetostrictive laminate (ME composit

23 force microscopy, we revealed coexistence of piezoelectric and non-piezoelectric phases in CuInP(2)Se

24 ncomitant with order-of-magnitude changes in piezoelectric and nonlinear optical responses.

25 nities arising from the coupling of ferroic, piezoelectric and optical responses.

26 static (curled) electric field, and superior piezoelectric and piezotoroidal responses, can be achiev

27 the semiconductors and generates substantial piezoelectric and pyroelectric effects.

28 trimethylamine borane can exhibit desirable piezoelectric and pyroelectric properties.

29 erator, derived from the simultaneous use of piezoelectric and triboelectric mechanisms in one press-

30 provides a new paradigm for designing highly piezoelectric and visible/near-infrared photoresponsive

31 rucial role in determining their dielectric, piezoelectric, and magnetoelectric properties.

32 A paradigm shift to piezoelectric antennas utilizing strain-driven currents

33 s paper describes a label-free and real-time piezoelectric aptasensor for the detection of cocaine.

34 simultaneously because most high-performance piezoelectrics are ferroelectrics that contain high-dens

35 Transparent piezoelectrics are highly desirable for numerous hybrid

36 Molecular piezoelectrics are highly desirable for their easy and e

37 canning probe microscopy (SPM) suggests that piezoelectric BaTiO(3) NPs display a coexistence of mult

38 ee acoustic transmitter that uses a flexible piezoelectric beam to harvest energy from fish swimming

39 a monoelemental 2D material predicted to be piezoelectric because of its highly directional properti

40 High-performance piezoelectrics benefit transducers and sensors in a vari

41 (-1), comparable to that of state-of-the-art piezoelectric bimorph cantilevers.

42 ons, future opportunities, and challenges of piezoelectric biomaterials for medical uses are reviewed

43 ening assays, corroborating the viability of piezoelectric biosensor as a cost-effective in vitro ass

44 chanism, namely electrochemical, optical and piezoelectric biosensors.

45 Modern piezoelectric biosensors/bioactuators are developed with

46 S) techniques, consisted of an array of four piezoelectric cantilevers with varying lengths to enhanc

47 This study highlights the potential of piezoelectric catalysis for overall water splitting.

48 Recently, piezoelectric characteristics have been a research focus

49 Their dielectric and piezoelectric characteristics peak near x = 0.5, but the

50 ites with augmented mechanical, thermal, and piezoelectric characteristics.

51 The materials with the highest piezoelectric charge coefficients (d (33)) are relaxor-P

52 oS2 devices can be actively modulated by the piezoelectric charge polarization-induced built-in elect

53 he magnitude of the stress and the resulting piezoelectric charges.

54 -dependent healing of artificial wounds on a piezoelectric chip for different cell lines.

55 We obtained a giant effective piezoelectric coefficient [Formula: see text] of ~1098 p

56 rate near-perfect transparency, an ultrahigh piezoelectric coefficient d(33) (greater than 2,100 pico

57 The piezoelectric coefficient d33 and remnant polarization P

58 tric effect, molecular piezoelectrics with a piezoelectric coefficient d33 comparable with piezoceram

59 n good agreement with the differences in the piezoelectric coefficient due to the electromechanical c

60 into a strained layer with an extremely low piezoelectric coefficient of 2.4 pm/V and a relaxed laye

61 cient of 2.4 pm/V and a relaxed layer with a piezoelectric coefficient of 32 pm/V.

62 A piezoelectric coefficient of d(33) ~10-16 pC N(-1) , and

63 energy at room temperature and a very small piezoelectric coefficient.

64 light on the physical origin of the highest piezoelectric coefficients as well as the softest elasti

65 their defining properties, such as ultrahigh piezoelectric coefficients, high permittivity over a bro

66 quire piezoelectric nanostructures with high piezoelectric coefficients.

67 soliton microcomb actuation using integrated piezoelectric components(13).

68 - xPbTiO3 (PMN-PT) nanobelt with a superior piezoelectric constant (d33 = ~550 pm/V), which is appro

69 nearly proportional to BNNT wt%, achieving a piezoelectric constant (|d(33) |) of 18 pmV(-1) at 9 wt%

70 efects are not the dominant contributor, the piezoelectric constant d33 and the remnant polarization

71 in two opposite directions with an effective piezoelectric constant d33 reaching 17.9 pm V(-1).

72 a0.7Ca0.3TiO3 (BZT-xBCT) system, the highest piezoelectric d33 coefficient appears at the tetragonal

73 piking mechanoreceptor system with a passive piezoelectric device as the tactile sensor.

74 s potential and hence the demonstration of a piezoelectric device remains lacking.

75 earch directions of flexible and stretchable piezoelectric devices are then discussed.

76 ar cells harvesting solar energy, tribo- and piezoelectric devices harvesting mechanical energy, and

77 Here, we develop conformal and piezoelectric devices that enable in vivo measurements o

78 n attempted to various applications, such as piezoelectric devices, energy harvesting devices, self-p

79 work allows the rational design of flexible piezoelectric devices, including flow-driven energy harv

80 Low-cost piezoelectric devices, such as simple frequency monitori

81 erials including shape memory alloys (SMAs), piezoelectrics, dielectric elastomer actuators (DEAs), i

82 y detected in the nozzle of the microfluidic piezoelectric dispenser chip to ensure printing of dropl

83 Using piezoelectric dispensing, two independent streams of ~50

84 act diffraction resolution through localized piezoelectric distortions of the lattice.

85 In addition, we were able to improve the piezoelectric effect by 1.85 times from 40 +/- 2 to 74 +

86 nt of the strain gradient is attributed to a piezoelectric effect driven by a transient screening fie

87 terials use both the pyroelectric effect and piezoelectric effect for energy conversion.

88 A piezoelectric effect observed in perovskite single-cryst

89 The local piezoelectric effect varies greatly within the tweed pat

90 ve passed since the discovery in 1880 of the piezoelectric effect, molecular piezoelectrics with a pi

91 ty, including a striking magnetically driven piezoelectric effect.

92 -mechanical coefficient which induces a high piezoelectric effect.

93 echanisms, novel techniques to produce their PIEZOelectric effects during the catalytic process, and

94 moelastic, deformation potential, or inverse piezoelectric effects.

95 y-active SiC quantum defects driven by local piezoelectric effects.

96 y is single cell isolation via small droplet piezoelectric ejection followed by capture of the drople

97 emonstrate an ultra-low loss lithium niobate piezoelectric electric dipole driven at acoustic resonan

98 onducting polymers; stimuli-responsive gels; piezoelectric, electrostrictive, magnetostrictive, and p

99 ) of optical power (depending on size of the piezoelectric element and light wavelength spectrum).

100 Microcantilever arrays are driven by a piezoelectric element, and resonance frequencies and qua

101 mask-less 3D printed strain gauges, flexible piezoelectric energy harvester for powering the sensors

102 Piezoelectric energy harvester scavenges mechanical vibr

103 Piezoelectric energy harvesters are ideal candidates to

104 e above issues, we devise a novel integrated piezoelectric energy harvesting device that is structure

105 Therefore, the development of highly piezoelectric ferroelectric semiconductor remains challe

106 ze dependence observed in the dielectric and piezoelectric/ferroelectric properties.

107 n via the inverse magnetostriction effect in piezoelectric/ferromagnet heterostructures holds promise

108 in-coupled magnetoelectric (ME) phenomena in piezoelectric/ferromagnetic thin-film bilayers are a pro

109 We also demonstrate that these piezoelectric fiber bundles can serve as ultra-flexible

110 poly(vinylidene fluoride-trifluoroethylene) piezoelectric fiber bundles with a controlled separation

111 current is orthogonal to the strain-induced piezoelectric field.

112 ween the charge carriers in the GNRs and the piezoelectric fields associated with the SAWs being desc

113 agnetostrictive soft layers, fabricated on a piezoelectric film.

114 ic polarization of BaTiO3 is confirmed using piezoelectric force microscopy.

115 ing of a metallic NbN bottom electrode and a piezoelectric GaN film on a SiC substrate.

116 ing to their lack of ionic polarization, but piezoelectric generation is consistent with the non-cent

117 r by a small mechanical force and integrates piezoelectric generator into triboelectric generator, de

118 power electronics such as thermoelectric and piezoelectric generators, as well as optoelectronic devi

119 echnologies (i.e., resistive, capacitive, or piezoelectric) have yet offered a satisfactory solution

120 fold that of quartz MRs, indicating that the piezoelectric heterostructural catalysts display excepti

121 2D materials that are piezoelectric, i.e., that allow for a facile conversion

122 the qubit into a single phonon by means of a piezoelectric interaction(3) and subsequently converts t

123 We developed a piezoelectric intracochlear acoustic transducer (PIAT) d

124 sducers such as electrochemical, optical and piezoelectric is presented.

125 The implantation of a double piezoelectric layer inside the human body can, in the fu

126 .0, which was achieved by press-focusing the piezoelectric layer into a spherical curvature.

127 hin n-type ZnO layer deposited on the top of piezoelectric layer of FBAR to form a Schottky barrier.

128 s to US stimulation and composed by a double piezoelectric layer with different material composition

129 ide (MoO(2) ) flakes that exhibit unexpected piezoelectric-like response are fabricated, as MoO(2) is

130 rain-mediated multiferroic composites, i.e., piezoelectric-magnetostrictive heterostructures, hold pr

131 ectify electrical charges generated from the piezoelectric material because of its adaptable conducta

132 using energy loss on the same surface of the piezoelectric material can be minimized.

133 Utilizing the piezoelectric material LiTaO(3) 36 degrees XY-cut with a

134 a layer of quantum dots (QDs) and a layer of piezoelectric material.

135 e include the exploration of new stretchable piezoelectric materials (e.g., hybrid composite material

136 y property and origins of giant responses of piezoelectric materials (PbTiO3, BiFeO3).

137 Together, these advancements in the field of piezoelectric materials and microsystems can spark a new

138 evelopments in new intrinsically stretchable piezoelectric materials and rigid inorganic piezoelectri

139 e representative applications of stretchable piezoelectric materials and structures in wearable and i

140 Intriguingly, some piezoelectric materials are biodegradable in nature, whi

141 First, the PIEZOelectric materials are briefly introduced.

142 Biomolecular piezoelectric materials are considered a strong candidat

143 High-performance piezoelectric materials are critical components for elec

144 Commercial lead-based piezoelectric materials raised worldwide environmental c

145 on the number of available pyroelectric and piezoelectric materials remain a major limitation as 22

146 he discussion of theoretical modeling of the piezoelectric materials to convert mechanical deformatio

147 On the other hand, piezoelectric materials were employed to control magneti

148 Single-phase oxide piezoelectric materials with giant piezoelectric voltage

149 piezoelectric materials and rigid inorganic piezoelectric materials with novel stretchable structure

150 y modulate the shallow electric potential in piezoelectric materials.

151 bioactuators that are based on biocompatible piezoelectric materials.

152 void the toxicity of conventional lead-based piezoelectric materials.

153 ers, respectively, in sharp contrast to bulk piezoelectric materials.

154 s strong as that observed in conventional 2D piezoelectric materials.

155 received attention as nonlinear optical and piezoelectric materials.

156 The present study employed a non-invasive piezoelectric measure of sleep wake cycles in young, mid

157 (3)](0.7)-[PbTiO(3)](0.3) (PMN-PT) unclamped piezoelectric membranes with ferromagnetic Ni overlayers

158 ons, simultaneous chronoamperometry (CA) and piezoelectric microgravimetry (PM) measurements were per

159 ncy peaks, resulting from the operation of a piezoelectric micropump, are eliminated using the Ag lay

160 n of magnetic anisotropy in magnetostrictive/piezoelectric multiferroic heterostructures has been dem

161 lectrospinning polyvinylidenefluoride (PVDF) piezoelectric nanofiber tip links.

162 n of its application in energy scavenging, a piezoelectric nanogenerator (PNG) is built on the single

163 nly including two key technologies: flexible piezoelectric nanogenerators (PENGs) and flexible triboe

164 e of the arts of wearable fiber/fabric-based piezoelectric nanogenerators and triboelectric nanogener

165 Fabrication of soft piezoelectric nanomaterials is essential for the develop

166 mechanical resonances in a single ultrathin piezoelectric nanoplate.

167 devices scavenging mechanical energy require piezoelectric nanostructures with high piezoelectric coe

168 The piezoelectric nature of a single nanofiber tip link is c

169 Finally, the combined stretchable and piezoelectric nature of the composite was exploited to p

170 Ferroelectric piezoelectric nature of the films was confirmed from a s

171 Our piezoelectric needle sensor reveals mechanical heterogen

172 cal (amperometric, potentiometric), thermal, piezoelectric, optical (fluorescence, Surface Plasmon Re

173 ations require large and tunable dielectric, piezoelectric or pyroelectric response of ferroelectrics

174 esting another dominant mechanism, such as a piezoelectric or space-charge scattering.

175 This hybrid generator combines high piezoelectric output current and triboelectric output vo

176 ly observed that a double-clamped "flexible" piezoelectric P(VDF-TrFE) thin belt, when driven into th

177 wireless data transfer hardware powered by a piezoelectric patch is implemented to demonstrate self-p

178 negative capacitance circuits to an array of piezoelectric patches (sensors).

179 ) Oe(-1) is achieved in a heterostructure of piezoelectric Pb(Zr,Ti)O3 (PZT) film deposited on magnet

180 (FM) layer induces an elastic stress in the piezoelectric (PE) layer, which generates a PE potential

181 d PVDF/DA NFs exhibit significantly enhanced piezoelectric performance and excellent stability and bi

182 evealed coexistence of piezoelectric and non-piezoelectric phases in CuInP(2)Se(6), forming unusual d

183 Here we propose a thin piezoelectric plasmonic metasurface forming the resonant

184 al gene directly from patient stools using a piezoelectric plate sensor (PEPS) in conjunction with a

185 of phosphorene have explained the origin of piezoelectric polarization among P atoms.

186 ee-way coupling of semiconductor properties, piezoelectric polarization and optical excitation in ZnO

187 Applying a local pressure can generate piezoelectric polarization charges at the two ends of th

188 Utilizing the piezoelectric polarization created at the metal-MoS2 int

189 integrated GaN microcantilever that utilizes piezoelectric polarization-induced changes in two-dimens

190 h as graphene, semiconducting materials, and piezoelectric polymers.

191 poling, which is competitive with commercial piezoelectric polymers.

192 r (TMEG) arrays, composed of soft magnet and piezoelectric polyvinylidene difluoride (PVDF) cantileve

193 surrounding the quartz MR surfaces, and the piezoelectric potential (piezopotential) effectively fac

194 thod (to estimate free-fluid pressure) and a piezoelectric pressure catheter transducer (which is cap

195 a microfluidic system was developed using a piezoelectric pressure-driven fluid delivery system and

196 les calculations to determine that the giant piezoelectric properties arise from the enhanced local s

197 dition of Er(3+) to PVDF is shown to improve piezoelectric properties due to the formation of a self-

198 gions to the room-temperature dielectric and piezoelectric properties is in the range of 50-80%.

199 Employing the high piezoelectric properties of BaTiO(3) NPs, we demonstrate

200 tissue development and regeneration, and the piezoelectric properties of biological materials in the

201 sed here also shows a way to investigate the piezoelectric properties of other materials on the nanos

202 ution of polar nanoregions to the underlying piezoelectric properties of relaxor ferroelectrics has y

203 ite materials exhibit both semiconductor and piezoelectric properties under strains due to the non-ce

204 lline growth and the local ferroelectric and piezoelectric properties were evaluated by piezoresponse

205 s such as MoS2 show promising electronic and piezoelectric properties, but their low mechanical stren

206 center of symmetry, is predicted to exhibit piezoelectric properties, yet experimental evidence is l

207 ctromechanical systems due to their superior piezoelectric properties.

208 ningful measurement of the ferroelectric and piezoelectric properties.

209 s along a nonpolar direction can enhance its piezoelectric properties.

210 al material development is to achieve a high piezoelectric property with long-term stability in a bio

211 Here, a self-powered piezoelectric pulse sensor is demonstrated to enable in

212 We describe a piezoelectric pumping system for studying the mechanobio

213 Miniaturized, battery-powered piezoelectric pumps are utilized to drive the heat carry

214 polarization, can influence the dielectric, piezoelectric, pyroelectric and electronic properties of

215 filler-matrix interfaces on the dielectric, piezoelectric, pyroelectric, and electrocaloric properti

216 , an important class of materials, including piezoelectric, pyroelectric, and ferroelectric semicondu

217 ral energy conversion mechanisms such as the piezoelectric, pyroelectric, and thermoelectric effect a

218 ectrolytes, opto-electronics, ferroeletrics, piezoelectrics, pyroelectrics, barocalorics, magnetics,

219 uipped with periodically arranged and bonded piezoelectric (PZT) patches, resulting in two Dirac cone

220 Here we report on hybrid piezoelectric (PZT)/ferromagnetic (Co2FeAl) devices in w

221 e proof-of-concept work, multichannel series piezoelectric quartz crystal (MSPQC) was utilized as det

222 ) technique, and HMF was quantified, using a piezoelectric quartz crystal with gold electrodes coated

223 A piezoelectric radiating element eliminates the need for

224 icient is the highest achieved in the linear piezoelectric regime and expected to be stable for a wid

225 modulation, as we believe can be enabled by piezoelectric-resonance devices, is yet to be investigat

226 The combination of nanoplasmonic and piezoelectric resonances allows the proposed device to s

227 brid platform that integrates nanomechanical piezoelectric resonators with a microwave superconductin

228 an ultra-low hysteresis along with enhanced piezoelectric response (d33 ~ 190pC/N) and high temperat

229 igning BNNTs, which enhances the composites' piezoelectric response approximately five times.

230 thermal conductivity and furthermore tunable piezoelectric response by varying BNNT wt% and applied s

231 Here, we demonstrate that the piezoelectric response can change discontinuously across

232 years, the main strategy for obtaining large piezoelectric response has been to construct multiphase

233 n plays an important role in achieving large piezoelectric response in a domain motion-confined mater

234 We observed a finite and zero piezoelectric response in MoS(2) in odd and even number

235 The jump of the piezoelectric response is found to exist for all these t

236 esolved X-ray microdiffraction analyses, the piezoelectric response of the BiFeO3 film was resolved i

237 ure, can explain the abrupt amplification of piezoelectric response of the system near MPB.

238 o couple flexural deformation and transverse piezoelectric response.

239 , forming unusual domain walls with enhanced piezoelectric response.

240 and reveals their ubiquitous relation to the piezoelectric response.

241 ogies, finding lead-free materials with high piezoelectric responses constitutes an important current

242 ution of polar nanoregions to the dielectric/piezoelectric responses of relaxor-ferroelectric crystal

243 urthermore, BNNT/PDMS composites demonstrate piezoelectric responses that are linearly proportional t

244 It is found that charges from piezoelectric scaffolds can induce mineralization from s

245 Here, we report the concept of a gradient piezoelectric self-sensing system by integrating shuntin

246 formance observed with these metal/insulator/piezoelectric semiconductor PTJs suggest their great pot

247 In these metal/insulator/piezoelectric semiconductor PTJs, such as Pt/Al(2) O(3)

248 nation of physical and chemical phenomena in PIEZOelectric semiconductors has triggered much interest

249 ptical excitation in ZnO, GaN, CdS and other piezoelectric semiconductors leads to the emerging field

250 enhance the light emission of LEDs based on piezoelectric semiconductors through applying static str

251 dvances in the synthesis and applications of PIEZOelectric semiconductors, an important class of mate

252 including the introduction of representative PIEZOelectric semiconductors, their possible catalytic m

253 Hence, a highly sensitive and selective piezoelectric sensor for mel has been reported here via

254 The inorganic piezoelectric sensor on an ultrathin plastic achieves co

255 A ferroelectric BaTiO(3) -based pyro-piezoelectric sensor system is demonstrated to detect te

256 An autoantigen piezoelectric sensor to quantify specific circulating au

257 rer in a mechanical meta-layer that exploits piezoelectric sensor-actuator pairs controlled by digita

258 able structures for flexible and stretchable piezoelectric sensors and energy harvesters.

259 A rapid surge in the research on piezoelectric sensors is occurring with the arrival of t

260 The piezoelectric sensors used for the detection of human pa

261 In this work, piezoelectric sensors were previously coated with thin f

262 crystal microbalances (QCMs) to form the gas piezoelectric sensors.

263 s, Piezo-Force Microscopy (PFM) and Resonant Piezoelectric Spectroscopy (RPS).

264 pired by and derived from a common household piezoelectric stove lighter.

265 nging due to the large reduction of in-plane piezoelectric strain by substrate clamping, and in two-t

266 ge coefficient g33 originates from maximized piezoelectric strain coefficient d33 and minimized diele

267 limitations can be overcome by designing the piezoelectric strain tensor using the boundary interacti

268 -temperature antiferromagnet MnPt induced by piezoelectric strain.

269 Overall, we demonstrate a piezoelectric, strain-controlled AFM memory that is full

270 ouples the acoustic energy of the SAW on the piezoelectric substrate through a fluid coupling layer a

271 A piezoelectric substrate transfers electric field induced

272 ination of anisotropy and orientation of the piezoelectric substrate without the requirement for soph

273 pendicular magnetic anisotropy (PMA) and one piezoelectric substrate.

274 Surface acoustic waves (SAWs) propagating on piezoelectric substrates offer a convenient, contactless

275 Traditionally, SAWs have been generated on piezoelectric substrates, although the cost of the mater

276 Here, we introduce the use of a piezoelectric system called Smart-touch fine needle (or

277 First, we used a piezoelectric system validated for Mus musculus to monit

278 uoride copolymers is analyzed and their full piezoelectric tensors are provided.

279 show that such reconstruction creates strong piezoelectric textures, opening a new avenue for enginee

280 yzing instability and nonlinear behaviors of piezoelectric thermal nano-bridges.

281 actuator has a silicon diaphragm driven by a piezoelectric thin film (e.g., lead-zirconium-titanium o

282 consists of mass-manufacturable, conformable piezoelectric thin films for strain mapping; multiphysic

283 otrophic lateral sclerosis, we show that the piezoelectric thin films, coupled with algorithms for th

284 (ME) antennas with a suspended ferromagnetic/piezoelectric thin-film heterostructure.

285 strate that when integrated with a miniature piezoelectric transducer the proposed sensor-data-logger

286 T), droplets are produced by focusing pulsed piezoelectric transducer-generated acoustic waves at the

287 The implants consist of piezoelectric transducers measuring 2 x 2 x 2 mm(3) and

288 Experiments employed piezoelectric transducers to excite and detect longitudi

289 -1.0 nm)/Pt thin films by strain applied via piezoelectric transducers.

290 gly coupled to a superconducting qubit using piezoelectric transduction with a cooperativity of 260.

291 avenge mechanical and thermal energies using piezoelectric, triboelectric, and pyroelectric effects.

292 proaches to be covered include pyroelectric, piezoelectric, triboelectric, flexoelectric, thermoelect

293 EA microprobe consists of a millimeter-sized piezoelectric ultrasonic receiver, a rectifier circuit,

294 ase oxide piezoelectric materials with giant piezoelectric voltage coefficient (g, induced voltage un

295 ase field simulations confirm that the large piezoelectric voltage coefficient g33 originates from ma

296 ic fields of electromagnetic waves, giving a piezoelectric voltage output.

297 rnal acoustic stimulus can be sensed via the piezoelectric voltage response of the implanted MEMS tra

298 ine ferroelectrics, a prototypical lead-free piezoelectric with an ambiguous switching mechanism.

299 1880 of the piezoelectric effect, molecular piezoelectrics with a piezoelectric coefficient d33 comp

300 Herein is an example of using piezoelectric ZnO nanoparticles to generate free-radical