ライフサイエンスコーパス: vibration

1 open-circuit voltage of 42 V under a 0.25 Hz vibration.

2 urned on and delivered a slow heartbeat-like vibration.

3 ate phase separation in a granular gas under vibration.

4 gap is partially out of phase with the plate vibration.

5 e sebaceous glands in vivo, using mechanical vibration.

6 ed to point measurements of basilar membrane vibration.

7 ant to movement, protecting it from external vibration.

8 f an (18)O(2)-sensitive resonance Raman (rR) vibration.

9 tion in solid state introduced by ultrasonic vibration.

10 sure changes and to high frequency sound and vibration.

11 ted voice fundamental frequency into tactile vibrations.

12 at rapidly open in response to sound-induced vibrations.

13 nt way to modify the energetics of molecular vibrations.

14 focussed on the microscopic details of these vibrations.

15 ways due to the presence of -OH, -NH and -CH vibrations.

16 chaotic pattern and less pronounced bending vibrations.

17 led by Raman scattering studies of water O-H vibrations.

18 led nonadiabatically to local intramolecular vibrations.

19 f near infrared radiation (NIR) by molecular vibrations.

20 nator's ability to resolve thermally induced vibrations.

21 nances (LSPR) can be resonant with molecular vibrations.

22 ity or using heat mirrors to reflect thermal vibrations.

23 ted by the selective excitation of molecular vibrations.

24 fields (tip-induced plasmons), and molecular vibrations.

25 differences in the nu(C=O) and nu(C-H) band vibrations.

26 d effects of aging, chemical treatments, and vibrations.

27 ponding conversion of photoenergy to lattice vibrations.

28 high temperatures is due to local molecular vibrations.

29 trong coupling between magnetism and lattice vibrations.

30 ining USV production: superficial vocal fold vibrations [2], and a hole-tone whistle [3].

31 n applications of flexible conductors, shock/vibration absorbers, thermal shock barriers, thermal ins

32 Coherent lattice vibrations (acoustic phonons) govern thermal transport i

33 Excited vibrations affect predominantly trapped carriers.

34 Periodic vibration also increased the dissipation rate of four pe

35 When paired with tACS, muscle tendon vibration also induced elevations of CSE.

36 indicative of multiple binding tethers, (2) vibration amplitudes of adhering bacteria parallel to a

37 etween previously published basilar membrane vibration and auditory nerve single unit data.

38 lexible 2D insulators with anomalous lattice vibration and chemical and physical properties.

39 The effect depends on the nature of the vibration and its mode-specific character can be well de

40 ics to detect and discriminate light, sound, vibration and other signals.

41 iving cochlea that increase the amplitude of vibration and sharpen frequency tuning, the data have ty

42 ion time for bimodal stimuli (i.e. when both vibration and sound were perceived).

43 he two structures and the observed torsional vibration and supports the prediction that the D2d symme

44 to 2.9 micrometres--where the OH stretching vibration and the H2O bending overtone are found--has pr

45 Findings support the use of both mechanical vibration and topical anesthetic as effective in childre

46 Tympanal vibrations and auditory nerve responses reveal that loca

47 orld materials are never perfect, as thermal vibrations and defects introduce significant deviation f

48 ectric energy harvester scavenges mechanical vibrations and generates electricity.

49 structural damage from shocks, environmental vibrations and oscillatory stress can be made using biom

50 beam, we measure the beam's thermally driven vibrations and perturb its motion with optical force flu

51 length, marks the boundary between molecular vibrations and phonons.

52 energy as a descriptor for certain molecular vibrations and rigorously relate errors in frequencies t

53 these vibrations involve unique rigid-chain vibrations and S-S molecular oscillations.

54 Thermal vibrations and the dynamic disorder they create can detr

55 ssignment of the molecular identity of these vibrations and their biological importance has not yet b

56 One can envision using the subsurface vibrations and their coupling across the interface to tr

57 These experiments demonstrate subsurface vibrations and their coupling to solvent and electron dy

58 attributed to the deformation and stretching vibration, and bending vibration of the OH group of wate

59 to the directionality of the intramolecular vibrations, and immediately resolve the inconsistency be

60 ize finger movement, hand gestures, acoustic vibrations, and real-time pulse wave.

61 do produce force, but that their effects on vibration are small and do not sharpen tuning.

62 etween reticular lamina and basilar membrane vibrations are absent in postmortem cochleae.

63 ublished data on proteins where only thermal vibrations are active.

64 lculations indicate that the low-energy Caxy vibrations are critical to the pairing, and that it shou

65 e interactions between electrons and lattice vibrations are fundamental to materials behaviour.

66 The CO stretch vibrations are very sensitive to the redox changes withi

67 found to well correlate with the low energy vibrations as determined by THz spectroscopy.

68 the dominance of antisymmetric CH methylene vibrations as the anhydrous milk fats crystal lattice be

69 erimental/theoretical evidence for sustained vibration-assisted electronic (vibronic) coherence in th

70 odulation affected both local, fast, protein vibrations associated with the catalyzed chemistry and t

71 ) with respect to the as-adsorbed CN/Au{111} vibration at 2146 cm(-1) is observed.

72 rum of complex 1 reveals the Fe-O stretching vibration at 832 +/- 3 cm(-1).

73 t the best frequency, and results in maximal vibration at the apical ends of outer hair cells.

74 Resonance Raman spectroscopy shows two Cu-S vibrations at 425 and 413 cm(-1), the latter with a -3 c

75 ns and non-invasively measured sound-induced vibrations at four locations distributed over the apical

76 lysis sheds light on the nature of localized vibrations at interfaces and can be enlightening for oth

77 We found a distinguishable C-D vibration band at 2070-2300 cm(-1) in single-cell Raman

78 Raman spectrum of 2 reveals a diatomic Co-O vibration band at 770 cm(-1), which provides the conclus

79 90.4289 cm(-1); part of the corresponding v4 vibration band has been measured with Doppler-limited re

80 um which is in resonance with the OH stretch vibration band of solvents like water and alcohols.

81 small size of nanomechanical systems, their vibrations become nonlinear already for small amplitudes

82 bond after proton transfer undergoes several vibrations before heavy-atom motion completes the reacti

83 studies of diatomic molecules that molecular vibration can be strongly coupled to electrons of the me

84 e lower strain rate regime, it is found that vibrations can be used to control jamming and granulatio

85 restitution grains, subject to low-amplitude vibration, can serve as experimentally-accessible analog

86 noparticles, which under external mechanical vibration caused cell lysis and released DNA in the supe

87 odification of the excited-state kinetics of vibration-cavity polariton systems.

88 the direct measurement of the lifetime of a vibration-cavity polariton.

89 bi oscillations, between the upper and lower vibration-cavity polaritons.

90 e, we present direct numerical evidence that vibrations change nature at a well-defined location deep

91 tion of reticular lamina to basilar membrane vibration changes with frequency by up to 180 degrees fr

92 en sublaminates, which eventually alters the vibration characters of the four-sublaminate lamina in m

93 The outer hair cell-driven reticular lamina vibration collaboratively interacts with the basilar mem

94 avy enzyme" effect demonstrates that protein vibrations contribute to catalysis in PETNR.

95 he role of elastography in CLDs, focusing on vibration-controlled transient elastography (VCTE) and m

96 of magnetic resonance (MR) elastography and vibration-controlled transient elastography (VCTE) in th

97 atients, coinfection and liver health tests, vibration-controlled transient elastography (VCTE), and

98 Vibration-controlled transient elastography estimates li

99 Vibration-controlled transient elastography for estimati

100 However, prior vibration-controlled transient elastography studies repo

101 ins followed by significant changes in Raman vibrations corresponding to aromatic amino acids such as

102 tly, we demonstrate that the strong electron-vibration coupling is essential to properly describe the

103 mond cages, called diamondoids, the electron-vibration coupling leads to the breakdown of the electro

104 findings reflect the dependence of electron/vibration coupling on the metallic nature, size and surf

105 rgetic - and from inherently strong electron-vibration couplings.

106 both directions of movement: thus, twice per vibration cycle.

107 ative sensory symptoms at onset; significant vibration deficits; and a non-length dependent progressi

108 regulated by merely controlling its coupling vibrations, depending on its structure size.

109 ir cells do not amplify the basilar membrane vibration directly through a local feedback as commonly

110 In this study, by measuring subnanometer vibrations directly from the reticular lamina at the api

111 endoprosthesis induced by static forces and vibrations during daily activities can potentially promo

112 implication of this finding spans across the vibration dynamics and transducer application spectrum,

113 Many nontrivial aspects of the vibration dynamics arise from the coexistence of several

114 In contrast, the lack of vibration-electron coupling on approximately 1 nm partic

115 Calculations have indicated protein vibrations enable structural change.

116 umulative operational frequency bandwidth of vibration energy harvesting for enabling self-powered mi

117 A versatile vibration energy harvesting platform based on a triboele

118 so that voltage and spiking mainly track the vibration envelope rather than individual cycles.

119 timulation and somatosensory physiology with vibration-evoked electroencephalographic potentials.

120 which is additionally sensitive to substrate vibration, feeds this information back to the brain via

121 to demonstrate the effectiveness of periodic vibration for strongly hydrophobic compounds such as hex

122 me-dependent changes in the intensity of the vibration frequencies of molecules that appear or disapp

123 TMEGs were shown to achieve high vibration frequency at small temperature gradients, ther

124 to moderate hydrogen bond with a C-H stretch vibration frequency blue-shifted by 14 cm(-1) and d(F-H)

125 It is found that the vibration frequency is an eigenvalue of the delaminated

126 main variables affecting range of vocal fold vibration frequency, namely vocal fold elongation and ti

127 ted from the area under the naphthalene ring vibration from propranolol was 133.1 ng/mL (0.45 muM), 1

128 tion stimulus-thus, perceived intensity of a vibration grew over the course of hundreds of millisecon

129 e intermediate-frequency wagging and bending vibrations have more contribution to electron-phonon cou

130 ments, suggests the potential use of elastic vibrations (i.e., phonons) in information processing, fo

131 suggesting relevant time scale(s) for those vibrations implicated in the "heavy enzyme" isotope effe

132 given the relative imprecision of vocal fold vibration in desiccated versus humid contexts, arid and

133 We tested the ability of the tag to measure vibration in excised whiskers in a flume in response to

134 he dynamics of the ester carbonyl stretching vibration in hydrated phosphocholine lipid bilayers, we

135 the recent development of optomechanics, the vibration in solids, involving collective motion of tril

136 to track the frequency of every O-D stretch vibration in the complex as the transferring hydron is i

137 igated the propagation patterns of cutaneous vibration in the hand during interactions with touched o

138 ormants"), rather than in the rate of tissue vibration in the sound source ("pitch").

139 e editing to monitor the CO/CN(-) stretching vibrations in [FeFe]-hydrogenase HYDA1 from Chlamydomona

140 osecond conversion of photoenergy to lattice vibrations in a model bilayered semiconductor, molybdenu

141 residues by monitoring their C=O stretching vibrations in H2O and in D2O.

142 Further, the excitonic nature of vibrations in neat H2O, which spans multiple water molec

143 e to synergetic enhancement effect of alkyne vibrations in Raman-silent region compared to alkyne-con

144 Non-linear gain, or amplification of the vibrations in response to low-intensity stimuli, was fou

145 We test the hypothesis that rainfall-induced vibrations in soil are the cues that trigger the emergen

146 Heavy enzymes have been used to test if the vibrations in the native enzyme are coupled to the chemi

147 l cortex revealed enhanced representation of vibrations in the prioritized context.

148 aterials with enhanced and distinctive Raman vibrations in the Raman-silent region (1800-2800 cm(-1)

149 n, sensitizing mast cells to IgE-independent vibration-induced degranulation.

150 are optomechanically characterized using the vibration-induced phase shift (VIPS) without detaching t

151 nerated force, which amplifies sound-induced vibrations inside the cochlea.

152 Here by directly measuring microstructure vibrations inside the cochlear partition using a custom-

153 Cochlear hair cells convert sound-induced vibration into electrical signals.

154 hanosensory cells that convert sound-induced vibrations into electrochemical signals.

155 , startling devices able to convert vertical vibrations into rotations of the device.

156 ional modes, and interestingly some of these vibrations involve unique rigid-chain vibrations and S-S

157 t sound frequencies because basilar membrane vibration is mechanically tuned to different frequencies

158 leae that the sound-induced reticular lamina vibration is substantially larger than the basilar membr

159 Since molecular vibration is the same motion needed for bond breaking, i

160 vibrations, yet how cellular forces amplify vibrations is poorly understood.

161 in-plane, whereas the amplitude of acoustic vibrations is used to control particle motion along an o

162 s are required, the energy dissipated by the vibrations is usually compensated by replenishment from

163 r various applications such as wave guiding, vibration isolation, or the design of static properties

164 Here, we utilized low intensity vibrations (LIV) as a physiologically relevant mechanica

165 cifically arising from the FMN suggests that vibrations local to the active site play a role in the h

166 The low-energy nature of these vibrations makes it difficult to access them experimenta

167 nt dependence on stimulus frequency than the vibrations measured near the mechanosensitive stereocili

168 However, recent progress in vibration measurement techniques reveals that organ of C

169 In accompanying with the macro vibration, micro buckles occur on the interfaces of the

170 esign heterogeneous composites for broadband vibration mitigation and impact resistance under mechani

171 ol elastic wave propagation are essential in vibration mitigation and sound attenuation.

172 terial and structural concepts for broadband vibration mitigation.

173 r-sublaminate lamina has a consistent global vibration mode.

174 near crossing), where the frequencies of two vibration modes get close to each other, to realize a ba

175 near elastic coupling between the degenerate vibration modes in a micromechanical disk-resonator, and

176 fect degeneracy of the primary and secondary vibration modes is achieved through electrostatic freque

177 Here, we report excitation of harmonics of vibration modes of solvent molecules by femtosecond lase

178 e electrostrictive layer, and resonant fibre vibration modes tunable under AC-driving conditions.

179 after 7, 14, 28, and 56 days under different vibration modes was compared to that under static and mi

180 engineering innovation of adapting low-cost vibration motors for periodically disrupting the depleti

181 le walking could be affected through mastoid vibration (MV) and changes are in the direction of motio

182 w manipulating sensory input through mastoid vibration (MV) could affect dynamic postural control dur

183 odel for the explanations of the acetone C=O vibration NCE phenomenon and its concentration effect.

184 oxyl was separately observed by a subsurface vibration near 800 cm(-1) from Ti-O located in the plane

185 pplications, including control of structural vibrations, noise, and shock mitigation.

186 bstantially larger than the basilar membrane vibration not only at the best frequency but surprisingl

187 ne wastes extracts were encapsulated through vibration nozzle microencapsulation using sodium alginat

188 ondon progression, we can determine the same vibration occurring at 616 +/- 10 cm(-1) in the E(dxy --

189 a multiscale approach to study the nonlinear vibration of fiber reinforced composite laminates contai

190 Periodic vibration of polyethylene (PE) passive samplers during e

191 cochlear physiology is that tuned mechanical vibration of the basilar membrane defines the frequency

192 at, after normalizing their responses to the vibration of the basilar membrane, the radial vibrations

193 lectivity by defining which OHCs enhance the vibration of the basilar membrane, thereby tuning the ga

194 avelling wave rather than an immediate local vibration of the basilar membrane; this travelling wave

195 ds following excitation of an intramolecular vibration of the cluster.

196 mation and stretching vibration, and bending vibration of the OH group of water physisorbed to TiO2,

197 O3/aqueous interface, we reveal a subsurface vibration of the oxygen directly below, and uniquely gen

198 (-1)) related to CH out of plane deformation vibration of trans double bond.

199 They are the resonant vibrations of a bridge demonstrating simultaneous spatia

200 tial and temporal modal analysis, micrometer vibrations of a metamaterial demonstrating wave propagat

201 mers are usually interpreted in terms of the vibrations of a structural repeat.

202 ater identified the symmetric and asymmetric vibrations of an Fe-O-Fe unit in the active site at 485

203 ing parameter than high-frequency stretching vibrations of H2 and H3.

204 al coupling between the picocavity field and vibrations of individual molecular bonds.

205 igned mainly to the symmetric CH2 stretching vibrations of lipids.

206 ational calculations reveal that the lattice vibrations of Mg(OH)2 have fundamentally different signa

207 py is a powerful tool for characterising the vibrations of molecular bonds and is therefore ideal for

208 Infrared vibrations of molecules located in these fields are enha

209 1340 cm(-1) due to the asymmetric stretching vibrations of nitrate.

210 Analysis of ethylenic and fingerprint vibrations of retinal provides evidence that the 13-cis

211 Here we show that the vibrations of seal whiskers may provide information abou

212 s among the first and third bending modes of vibrations of slightly curved beams (arches): two-one in

213 orce that greatly increases the sound-evoked vibrations of the basilar membrane.

214 ow that temperature-activated intramolecular vibrations of the ground state play a major role in dete

215 screte electronic transitions that couple to vibrations of the nanocrystal lattice.

216 In the mammalian cochlea, small vibrations of the sensory epithelium are amplified due t

217 ibration of the basilar membrane, the radial vibrations of the tectorial membrane and reticular lamin

218 Furthermore, analysis of the intermolecular vibrations of the water network reveals that retarded wa

219 pling between large-amplitude coherent optic vibrations of Tl-rattlers along the c-axis, and acoustic

220 ecular motions (i.e., molecular rotations or vibrations) of a flexible fluorescent probe can be signi

221 In contrast, a tactile stimulus (i.e. vibration on the skin) did not lead to a significant cha

222 ct experimental probe of the role of protein vibrations on enzyme-catalyzed reactions.

223 adolinium, was employed to obtain mechanical vibrations on the PVDF cantilever under small thermal gr

224 Intriguingly, this interfacial Ti-O stretch vibration, once decoupled from the lattice, couples to r

225 However, previous measurements found these vibrations only weakly depend on the functional state.

226 system geometry variations over time due to vibrations or temperature fluctuations.

227 Rats were trained to detect whisker vibrations or visual flickers.

228 electrodes; catalyst supports; and acoustic, vibration, or shock energy damping.

229 e antiresonances are observed when activated vibrations overlap with electronic transitions.

230 specifically probed by the oxyl's subsurface vibration, parallels that of the photocurrent.

231 The observed vibration patterns evolved rapidly in time, peaking in i

232 er-risk women exhibited significantly poorer vibration perception in the distal lower extremities (P

233 cale (coefficient = -3.78, 0.01 < P < 0.05), vibration perception thresholds (coefficient = -4.37, P

234 s were clinically assessed on grip strength, vibration perception thresholds and postural stability,

235 ward movement, meaning they are sensitive to vibration phase.

236 oss-section is strongly dominated by lattice vibrations (phonons).

237 ermined allowing for the analysis of the key vibrations playing a role in the band shapes.

238 ehydrogenase (LDH) employs protein promoting vibrations (PPVs) on the femtosecond (fs) to picosecond

239 tic interactions, but little is known of how vibrations propagate throughout the hand.

240 mapped and analyzed spatial distributions of vibrations propagating in the skin of the dorsal region

241 Using mechanical vibrations ranging from 0.1 to 6 kHz, we performed four

242 diffusion, molecular conformational changes, vibrations, reaction pathways and interface dynamics.

243 it could be a vibrational wave detected by a vibration receiver of another sort.

244 B1 cells) that are postsynaptic to antennal vibration receptors.

245 hermore, the extent to which the patterns of vibrations reflect the nature of the objects that are to

246 d rotation are quickly cooled, the molecular vibration relaxes at impractically long timescales.

247 pin-relevant mechanisms, the role of lattice vibration remains poorly understood.

248 External mechanical vibration repeats an oscillating motion of a polymer-coa

249 The system is also shock and vibration resistant, due to the multiple points of conta

250 oustic and optic modes arising from Ti and H vibrations, respectively, and frequencies of optic modes

251 We show that nitrile nu(C identical withN) vibrations respond to the degree of electron localizatio

252 eriments guided by simulations, how acoustic vibrations result in micromanipulations in a microfluidi

253 l modulus hardening due to anharmonic atomic vibration, resulting in a low and temperature-independen

254 Terahertz (THz) vibration-rotation-tunneling (VRT) spectroscopy resolved

255 ues sampled from a normal distribution; each vibration's mean speed was proportional to the width of

256 Detailed testing with a vibration sensitivity testing device in a subgroup of 47

257 For the fiber vibration sensor, the proposed numerical model shows tha

258 1), while rats compared the intensity of two vibrations separated by an interstimulus delay.

259 O-Au NPs) greatly enhanced the CO stretching vibration signal at 2100cm(-1), which is relatively fre

260 A unique bioassay allows a substrate-borne vibration signal to be isolated and manipulated to test

261 gh-frequency sounds that generates substrate vibrations similar to those produced by female lebinthin

262 cative gain control and enhanced response to vibration stimuli during the whisker session.

263 ker session, 80% of trials contained a brief vibration stimulus applied to whiskers and the remaining

264 nits responded differentially to the whisker vibration stimulus when presented with higher probabilit

265 for the disabled, because the simple throat vibrations such as hum, cough and scream with different

266 c transitions strongly couple to phonons and vibrations, such as energy transfer in photosynthetic pi

267 Sound vibration (SV), a mechanical stimulus, can trigger vario

268 ressed in this review are the intermolecular vibrations that are more directly probed by the low-freq

269 is often strongly coupled to intramolecular vibrations that can promote, suppress and direct electro

270 controls when exposed to low-frequency soil vibrations that closely mimic those of rainfall.

271 activation energy, and is likely due to fast vibrations that may be enabled by water mobility on the

272 e dermis of the skin, detects high frequency vibrations that occur within its large receptive field.

273 volume with dynamics information via atomic vibrations that probe local configurational space and in

274 uning the frequency and the amplitude of the vibration, the dimer undergoes either a directed motion

275 For the sinusoidal vibration, the output energy can be maximized by resonan

276 Under a 2.5 Hz vibration, the peak open-circuit voltage reached 115 V u

277 wding effect that stiffens the 2 degrees H/D vibrations, thus decreasing the 2 degrees KIE.

278 lays a critical damping effect on transverse vibrations, thus inhibiting negative thermal expansion.

279 A blue shift to higher frequencies of the CN vibration to 2235 cm(-1) with respect to the as-adsorbed

280 We found these spatial patterns of vibration to vary systematically with touch interactions

281 ments that support coupling of the promoting vibrations to barrier crossing and the coincidence of hy

282 us to identify the transition from molecular vibrations to bulk phonons in cadmium selenide quantum d

283 earned behaviours to generate high-frequency vibrations to release pollen from flowers with specialis

284 ifferent length scales, ranging from thermal vibrations to seismic excitation.

285 mittent aerobic exercise (IAE) or mechanical vibration training (MVT), for four weeks and examined th

286 ystems is the excitation of intrachromophore vibrations upon electronic excitation and energy transfe

287 nonlinearities to switch and amplify elastic vibrations, via magnetic coupling, operating at a single

288 s different from flapping and vortex-induced-vibration (VIV).

289 The amplitude of the incus vibration was found to be in the range between 10pm to 1

290 Vibrations were "noisy," constructed by stringing togeth

291 Repeated balance perturbations through calf vibrations were used to study postural adaptation.

292 ng correlated with the local features of the vibration, whereas vM1 firing correlated with the percep

293 steric hindrance of transverse fluoride ion vibrations, which directly controls the thermal expansio

294 eV, most likely due to coupling to a silica vibration with an energy that varies between 160 and 180

295 in aqueous solution by probing the acoustic vibrations with four-wave mixing.

296 ystemic manifestations in response to dermal vibration, with coincident degranulation of mast cells a

297 Here, we measured sound-induced vibrations within the apical half of the chicken basilar

298 ereocilia, arguing that the tuning of radial vibrations within the hair cell epithelium is distinct f

299 gin of tuning by measuring sound-induced 2-D vibrations within the mouse organ of Corti in vivo Our g

300 or amplifying sound-induced basilar membrane vibrations, yet how cellular forces amplify vibrations i