ライフサイエンスコーパス: piezoelectric

1 n nitride (C3N4) in its various forms is non-piezoelectric.

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

3 ign to optimize the performance of lead-free piezoelectrics.

4 oupled to strain, making ferroelectrics good piezoelectrics.

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

6 MN4 was evaluated using the electromagnetic piezoelectric acoustic sensor (EMPAS).

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

8 8) was formed on planar gold electrodes of a piezoelectric acoustic sensor.

9 retical characterization of the responses of piezoelectric actuator-sensor pairs laminated on a varie

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

11 n array of elastomeric tips mounted onto the piezoelectric actuators of an atomic force microscope.

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

13 o-integrated with nanophotonic resonators on piezoelectric aluminum nitride substrates.

14 Monolayer MoS2 is predicted to be strongly piezoelectric, an effect that disappears in the bulk owi

15 ibed in lower organisms, and thermoelectric, piezoelectric and biofuel devices are promising for mamm

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

17 al permittivity must be optimized to balance piezoelectric and capacitive effects.

18 ense non-volatile memories, nanoscale hybrid piezoelectric and charge sensors, as well as building bl

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

20 Here, we demonstrate that the piezoelectric and liquid-crystalline properties of M13 b

21 articular focus on electrochemical, optical, piezoelectric and magnetic based sensors.

22 ltilayer approaches involving strain-coupled piezoelectric and magnetostrictive components are the cl

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

24 ing enabled by good connectivity amongst the piezoelectric and magnetostrictive phases.

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

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

27 d on different physics, which combines known piezoelectric and piezoresistive materials, is described

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

29 Ultrathin inorganic piezoelectric and semiconductor materials on elastomer s

30 Recently, piezoelectric and triboelectric energy harvesting device

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

32 ubstitute for lead-based materials in future piezoelectric applications.

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

34 Molecular piezoelectrics are highly desirable for their easy and e

35 High-performance piezoelectrics are lead-based solid solutions that exhib

36 on GmbH, Ulm, Germany) were measured using a piezoelectric axial vibrator.

37 nergy storage devices and the fabrication of piezoelectric-based sensors.

38 g between magnetostrictive Ni electrodes and piezoelectric BaTiO(3)-based dielectric layers.

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

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

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

42 cherichia coli O157:H7 was developed using a piezoelectric biosensor-quartz crystal microbalance (QCM

43 topological insulators, thermoelectrics and piezoelectrics, but only 83 out of 483 of these possible

44 lution is among the most promising lead-free piezoelectric candidates; however, depolarization of the

45 Piezoelectric cantilever sensors are shown to exhibit se

46 erum is given using gold (Au)-coated dynamic piezoelectric cantilever sensors.

47 est as candidate replacements for lead-based piezoelectric ceramics.

48 The piezoelectric characteristics of nanowires, thin films a

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

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

51 The piezoelectric coefficient d33 and remnant polarization P

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

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

54 er than 100% enhancement of the longitudinal piezoelectric coefficient in PMN-xPT relative to that in

55 nd that the remanent polarization and direct piezoelectric coefficient increased up to 12.14 muC/cm(2

56 Quantitatively, an e11 piezoelectric coefficient of 0.758 C m(-2) is predicted

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

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

59 olybdenum disulphide (MoS(2)) and a measured piezoelectric coefficient of e(1)(1) = 2.9 x 10(-10) C m

60 ization value and 27% increase of the direct piezoelectric coefficient were observed in the film with

61 (001) SrTiO(3) template layer with superior piezoelectric coefficients (e(31,f) = -27 +/- 3 coulombs

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

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

64 quire piezoelectric nanostructures with high piezoelectric coefficients.

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

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

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

68 with weak extrinsic domain wall pinning, the piezoelectric control allows one to experimentally asses

69 udes and report a direct observation and the piezoelectric control of the Walker breakdown separating

70 Our analysis indicates a high piezoelectric coupling coefficient and a low electrical

71 l displacement of the LES was recorded using piezoelectric crystals.

72 7+/-0.08 cm; P<0.05) and regional stiffness (piezoelectric crystals; 14.70+/-2.08 versus 9.11+/-1.24;

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

74 Lead-based piezoelectrics demonstrate a large mechanical response,

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

76 echanical energy into electrical energy, and piezoelectric devices made of a variety of inorganic mat

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 This is assigned to the generation of piezoelectric dipoles in the ZnO nanorods, indicating th

82 s, besides electrosprays, are plasma ion and piezoelectric discharge plasma sources.

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

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

85 ntermediate low-symmetry phase with a strong piezoelectric effect arises.

86 l magnetoelectric effect resembles the large piezoelectric effect at the morphotropic phase boundary

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

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

89 A numerical model, coupling a piezoelectric effect in the solid substrate and acoustic

90 imental study of the theoretically predicted piezoelectric effect in triangle monolayer MoS2 devices

91 A piezoelectric effect observed in perovskite single-cryst

92 The local piezoelectric effect varies greatly within the tweed pat

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

94 hen modifies the FE polarization through the piezoelectric effect, on a timescale much faster than la

95 ty, including a striking magnetically driven piezoelectric effect.

96 We attribute the enhancement of piezoelectric effects to the contributions from the shel

97 Recently, the strain state of a piezoelectric electrode has been found to impact the ele

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

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

100 enerator by associating this actuator with a piezoelectric element.

101 an outstanding potential to be utilized for piezoelectric energy generation with a performance proba

102 ple and environmentally friendly approach to piezoelectric energy generation.

103 Piezoelectric energy harvester scavenges mechanical vibr

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

105 high-speed ferroelectric domain imaging and piezoelectric energy-harvesting devices.

106 s per square meter) and figures of merit for piezoelectric energy-harvesting systems.

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

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

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

110 Large-active-area piezoelectric fibers are presented here, which can be wo

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 To this end, we developed high-power-density piezoelectric flight muscles and a manufacturing methodo

114 The piezoelectric force microscopy (PFM) measurement at room

115 Piezoelectric force microscopy (PFM), x-ray diffraction,

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

117 ng a high-speed camera in combination with a piezoelectric force sensor.

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

119 Finally, we develop a phage-based piezoelectric generator that produces up to 6 nA of curr

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

121 asuring the electrode mass in real time with piezoelectric gravimetry.

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

123 The magnetic/piezoelectric heterostructure based RF NEMS magnetoelect

124 A triboelectric-pyroelectric-piezoelectric hybrid cell, consisting of a triboelectric

125 pended in buffer and then analyzed using the piezoelectric immunosensor modified with specific captur

126 A piezoelectric immunosensor was developed for the real-ti

127 ructure of GaAs however, results in a strong piezoelectric interaction between lattice acoustic phono

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

129 hanges observed in the PDFs are dominated by piezoelectric lattice strain and ionic polarizability, r

130 .0, which was achieved by press-focusing the piezoelectric layer into a spherical curvature.

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

132 chanical systems (MEMS) incorporating active piezoelectric layers offer integrated actuation, sensing

133 plate sensors (PEPSs) consisting of a highly piezoelectric lead magnesium niobate-lead titanate (PMN-

134 rmation also causes all ferroelectrics to be piezoelectric, leading to applications in sensors and hi

135 recently demonstrated using magnetostrictive/piezoelectric magnetoelectric heterostructures.

136 hough such characteristics can be created in piezoelectric-magnetostrictive composites, to date they

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

138 rochemical activity taking place between the piezoelectric material and its solution environment.

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

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

141 alpha-quartz is a piezoelectric material, it can be produced artificially

142 ofluidic chip consisting of a single crystal piezoelectric material.

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

144 0.5Bi0.5TiO3 (NBT) is a well-known lead-free piezoelectric material; however, it is often reported to

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

146 rdinary behaviours in oxides, as observed in piezoelectric materials at morphotropic phase boundaries

147 fect, dubbed piezocatalysis, is prominent in piezoelectric materials because the strain state and ele

148 Piezoelectric materials can convert mechanical energy in

149 Piezoelectric materials exhibit a mechanical response to

150 describe here a prototype biosensor based on piezoelectric materials functionalized with specific ant

151 We synthesized grain-oriented lead-free piezoelectric materials in (K0.5Bi0.5TiO3-BaTiO3-xNa0.5B

152 of genetically modified phages, phage-based piezoelectric materials potentially offer a simple and e

153 Commercial lead-based piezoelectric materials raised worldwide environmental c

154 Single-phase oxide piezoelectric materials with giant piezoelectric voltage

155 e for future experiments utilizing different piezoelectric materials, such as ZnO, BaTiO(3), PbTiO(3)

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

157 cate the effective solution to the lead-free piezoelectric materials.

158 ls are of great interest as high-performance piezoelectric materials.

159 is one of the most important and widely used piezoelectric materials.

160 presence of ambient vibrations by the use of piezoelectric materials.

161 electric, structural, lattice dynamical, and piezoelectric measurements on PZT and PMN-xPT, two nearl

162 metamaterial unit cell composed of a single piezoelectric membrane augmented by a nonlinear electron

163 s selected for the evolution of prestin as a piezoelectric membrane motor.

164 resonator of EQCM and a Pt electrode for the piezoelectric microgravimetry (PM) and capacitive impedo

165 for simultaneous chronoamperometry (CA) and piezoelectric microgravimetry (PM) determination of seve

166 se porphyrins served for recognition and the piezoelectric microgravimetry (PM) for analytical signal

167 ctrochemical impedance spectroscopy (EIS) or piezoelectric microgravimetry (PM) for label-free analyt

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

169 ant of the complex of the MIP cavity and FU, piezoelectric microgravimetry (PM) under both batch- and

170 or of 2.9 for the MIP film was determined by piezoelectric microgravimetry using ECQM.

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

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

173 lectrospinning polyvinylidenefluoride (PVDF) piezoelectric nanofiber tip links.

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

175 iboelectric nanogenerator and a pyroelectric-piezoelectric nanogenerator, is developed for highly eff

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

177 mechanical resonances in a single ultrathin piezoelectric nanoplate.

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

179 e demonstrated the capability to use aligned piezoelectric nanowire arrays as a highly accurate nano-

180 n sensing applications is vertically aligned piezoelectric nanowire arrays that allow facile interfac

181 Piezoelectric nanowires are promising building blocks in

182 Piezoelectric nanowires are robust and can be stimulated

183 no-electromechanical systems developed using piezoelectric nanowires have gained interest primarily f

184 d durability of harvesting materials such as piezoelectric nanowires have steadily improved, the volt

185 chanical and electromechanical properties of piezoelectric nanowires is reviewed with an emphasis on

186 that will pave the way for optimal usage of piezoelectric nanowires.

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

188 to many biophysical forces, and notably its piezoelectric nature, may reflect anion interactions wit

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

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

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

192 The average of piezoelectric output voltage was about -20 mV, while 5-1

193 was about -20 mV, while 5-10% of the NWs had piezoelectric output voltages exceeding -(0.15-0.35) V.

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

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

196 H(2) production behaviors of an oscillating piezoelectric Pb(Mg(1)/(3)Nb(2)/(3))O(3)-32PbTiO(3) (PMN

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

198 electrical excitations can be measured using piezoelectric PbZr(x)Ti(1-x)O(3) (PZT) nanoribbons, and

199 als, consisting of coupled ferromagnetic and piezoelectric phases, are of great importance in the dri

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

201 e, in situ DNA hybridization detection using piezoelectric plate sensors (PEPSs) consisting of a high

202 00 nm sized FeGa nanomagnets delineated on a piezoelectric PMN-PT substrate.

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

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

205 Using the piezoelectric polarization charges created at a metal-se

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

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

208 ructing the photoresponsive film on top of a piezoelectric poly(vinylidene difluoride) film, electric

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

210 The tip, controlled by a piezoelectric positioner operated in closed loop, is osc

211 h is mainly ascribed to the instability of a piezoelectric positioner.

212 the wurtzite structured ZnO, GaN and InN, a piezoelectric potential (piezopotential) is created in t

213 ntral symmetry, such as ZnO, GaN, and InN, a piezoelectric potential (piezopotential) is created in t

214 effect is about the use of the inner crystal piezoelectric potential to tune/control charge carrier g

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

216 e enhancements of both the ferroelectric and piezoelectric properties are attributed to the increase

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

218 d-oxide perovskites that display exceptional piezoelectric properties for pseudorhombohedral composit

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

220 he Ag nanoparticles on the ferroelectric and piezoelectric properties of Ag/poly(vinylidenefluoride-t

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

222 opy, we characterize the structure-dependent piezoelectric properties of the phage at the molecular l

223 e report the first experimental study of the piezoelectric properties of two-dimensional MoS2 and sho

224 ZnO is a wide band-gap semiconductor with piezoelectric properties suitable for opto-electronics,

225 extremely low drive voltage due to thin-film piezoelectric properties that rival bulk PMN-PT single c

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

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

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

229 ningful measurement of the ferroelectric and piezoelectric properties.

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

231 en fibrils and peptide nanotubes can display piezoelectric properties.

232 ctromechanical systems due to their superior piezoelectric properties.

233 cs, which describes the coupling between the piezoelectric property and semiconducting behavior and f

234 ements in the existing nonlinear optical and piezoelectric property coefficients.

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

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

237 coupling self-oscillating polymer gels to a piezoelectric (PZ) micro-electro-mechanical system (MEMS

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

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

240 col-based mixed surface chemistry imposed on piezoelectric quartz discs.

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

242 tic electromotility is modeled by linearized piezoelectric relations whereas the OHC hair-bundle mech

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

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

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

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

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

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

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

250 pole strength of the phage, hence tuning the piezoelectric response, by genetically engineering the m

251 inability to integrate materials with giant piezoelectric response, such as Pb(Mg(1/3)Nb(2/3))O(3)-P

252 of the apparent and experimentally verified piezoelectric response.

253 o couple flexural deformation and transverse piezoelectric response.

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

255 ntal and theoretical studies reveal enhanced piezoelectric responses in lead zirconate titanate that

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

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

258 tic standing wave (BAW) resonators made from piezoelectric semiconductor (PS) materials.

259 hen strain is applied, given the n-side is a piezoelectric semiconductor and the p-type side is non-p

260 le piezotronic devices based on RF-sputtered piezoelectric semiconductor thin films have been investi

261 ric semiconductor and the p-type side is non-piezoelectric semiconductor.

262 ial when they are in contact with a strained piezoelectric semiconductor.

263 catalysis process utilizing well-established piezoelectric, semiconductor, molecular orbital and elec

264 Piezoelectric semiconductors are an extremely important

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

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

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

268 The inorganic piezoelectric sensor on an ultrathin plastic achieves co

269 An autoantigen piezoelectric sensor to quantify specific circulating au

270 nvasively by chin electromyography, cervical piezoelectric sensor, and inductive respiratory plethysm

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

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

273 Piezoelectric size effects for ferroelectric materials a

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

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

276 lf-assembled thin films of phage can exhibit piezoelectric strengths of up to 7.8 pm V(-1).

277 ar layer, the large surface energy can cause piezoelectric structures to be thermodynamically unstabl

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

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

280 Piezoelectric switching is only possible up to 300 degre

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

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

283 duct of 1.61 x 10(13) Hz among the suspended piezoelectric thin film resonators reported to date.

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

285 cal spot diameter of 90 mum delivered from a piezoelectric transducer evoked stable responses with a

286 ace acoustic wave (SAW) device on a LiNbO(3) piezoelectric transducer for the transfer of nonvolatile

287 eshoe structure which can be stimulated by a piezoelectric transducer to generate vortices in the flu

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

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 tion of commercially available low-frequency piezoelectric tuning forks (QTFs) for endotoxin detectio

294 number of atomic layers produces oscillating piezoelectric voltage and current outputs, whereas no ou

295 zed the device, and we report the effects of piezoelectric voltage and sample flow rate on device per

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

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

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

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

300 1880 of the piezoelectric effect, molecular piezoelectrics with a piezoelectric coefficient d33 comp