ライフサイエンスコーパス: damp

1 FP-p65 knock-in cells NF-kappaB behaves as a damped oscillator able to synchronize to a variety of pe

2 c recovery, most strikingly illustrated by a damped oscillation of most core clock genes, including A

3 ree-dimensional shape is well described by a damped sinusoidal wave on the plane of the Milky Way wit

4 e anomalous diffusion is then described by a damped white noise process with memory, with analytical

5 umulation of cortical actin reminiscent of a damped oscillation.

6 o well-described statistically in terms of a damped random walk model.

7 Bipolar NEFO was a damped sine wave with 140 ns first phase duration at 50%

8 sents a high toughness of 370 MJ m(-3) and a damping capacity of 95%.

9 structure with vertical symmetry breaking, a damping-like SOT can deterministically switch a perpendi

10 ably, the Co25Fe75 epitaxial films exhibit a damping constant <1.4 x 10(-3), which is comparable to t

11 ted by encapsulating the ring resonator in a damping medium.

12 The antenna response drives active damping with a shorter delay (~20 ms) to stabilize this

13 tical cooling of the mechanics without added damping, an effect that has no optical analog.

14 iesii, causing cankers in trees of all ages, damping-off in seedlings, and mortality in cuttings and

15 sistent with the expected range for Akhiezer damping, and the dependence of Q on temperature and geom

16 is consistent with expectations for Akhiezer damping.

17 Although damping suppresses these excitations, it can be compensa

18 We demonstrate the algorithm on an amplitude damping channel using the IBM Qiskit quantum simulator a

19 re affected by the white noise and amplitude damping.

20 s evolving under the action of the amplitude damping noisy channel.

21 mping, thermoelastic dissipation, and anchor damping are not significant dissipation mechanisms for t

22 ental factors (pollen/flowers [P = .005] and damp air [P = .012]) were more common in asthma.

23 sues persisted but became desynchronized and damped in constant darkness.

24 scence, including reduced B cell genesis and damped immune responses.

25 relatively large spin-mixing conductance and damping-like SOT through spin Hall magnetoresistance and

26 contrasting the experimental dispersion and damping of PhPs, revealed by polariton interferometry us

27 r variations in the amplitude, frequency and damping of the oscillations.

28 ional wavepacket with a period of 249 fs and damping time of 0.63 ps is observed on the (5)T(2g) surf

29 spring networks characterized by Hessian and damping matrices.

30 lso show micromagnetically that the IDMI and damping also combine to modify the domain wall velocity

31 etry, showing in general both field-like and damping-like torques are generated.

32 k to extract the whisker Young's modulus and damping coefficient.

33 ss, storage modulus, shear loss modulus, and damping ratio were calculated for all animals.

34 of the BEC, which show pronounced peaks and damping around the quantum critical point.

35 ecific to individual nodes such as power and damping.

36 ls significant bandwidth renormalization and damping effects due to the strong correlation among Mn 3

37 the lattice dependent frequency response and damping offered by the various classes of hourglass meta

38 se of resonance frequency analysis (RFA) and damping capacity analysis (DCA).

39 Conclusion Liver stiffness and damping ratio measurements can extend hepatic MR elastog

40 n mechanical properties (local stiffness and damping) extracted using dynamic and quasi-static force

41 tive contributions of field-like torques and damping-like torques to the magnetization switching indu

42 es for the high-frequency sound velocity and damping coefficients, which we find to be a sensitive pr

43 We observe a large anti-damping torque in the YIG/Pt system, revealing its promi

44 in observed dissolved gas concentrations are damped and lagged with respect to equilibrium concentrat

45 ered as fully coherent plasmons and they are damped even in the optical limit, i.e. for small momenta

46 oxygen species (ROS) production, as well as damping of neutrophils by metoprolol, effectively inhibi

47 irected motion is a result of the asymmetric damping due to the size difference in the filling grains

48 horylated (p)-rC0C7-sc was less effective at damping contractile oscillations, results suggest that s

49 he observed energy transfer while NSET-based damping models provided better fits but could not reprod

50 ales up to several tens of nanometers before damping.

51 have reported a positive association between damp housing conditions and asthma, but little is known

52 These data suggest an association between damp housing conditions and childhood eczema symptoms, w

53 ics, from the edge of the transition between damped to sustained oscillations during wakefulness, to

54 Of particular interest, bulk damping decreases monotonically as the temperature decre

55 Gilbert damping are identified, namely bulk damping and surface damping.

56 ate broadband perfect acoustic absorption by damped resonances through inclusion of lossy porous medi

57 rgy optical modes with acoustic modes causes damping of heat carrying acoustic phonons to ultrasoft f

58 s, and the only one to consistently classify damped signals as highly periodic.

59 of guest ions or molecules plays a critical damping effect on transverse vibrations, thus inhibiting

60 ent FeNi nanowire may have less eddy current damping, which could make it an alternative candidate fo

61 count, either through a local size-dependent damping model or through the Generalized Nonlocal Optica

62 Depending on the strength of diffusive damping, the model exhibits complex growth patterns such

63 miting values predicted by the bulk Au Drude damping parameter.

64 heterogeneity and not from strong electronic damping associated with lossy plasmonic materials.

65 t defects are promising materials for energy damping applications.

66 ts; and acoustic, vibration, or shock energy damping.

67 The energy damping time in a mechanical resonator is critical to ma

68 amide methylation confers stability to ETP, damping the spontaneous formation of tri- and tetrasulfi

69 -exist, others where the populations exhibit damped oscillations, and still others where one populati

70 xtures undergo osmotic relaxation exhibiting damped oscillations in phase behavior, which is synchron

71 accounting for both intrinsic and extrinsic damping sources.

72 strained film structure suppresses extrinsic damping, enables soft magnetic behavior, and generates l

73 r noise at the single-cell results in faster damping at the population level.

74 the superfluid density and the normal fluid damping.

75 anchors, we have been able to show that gas damping, thermoelastic dissipation, and anchor damping a

76 Gilbert damping increases approximately linearly with increasing

77 ental study of temperature-dependent Gilbert damping in permalloy (Py) thin films of varying thicknes

78 ite thin films with an unusually low Gilbert damping parameter (<3 x 10(-3) ), as well as strong magn

79 ng against the equilibrium-restoring Gilbert damping of the magnetization dynamics.

80 two independent contributions to the Gilbert damping are identified, namely bulk damping and surface

81 While the Gilbert damping constant can reach 10(-4) to 10(-5) in some insu

82 nsight to the physical origin of the Gilbert damping in ultrathin magnetic films.

83 The Gilbert damping is found to be almost independent of the MgO thi

84 rstanding the physical origin of the Gilbert damping is highly relevant to developing future fast swi

85 The Gilbert damping of ferromagnetic materials is arguably the most

86 -mode damped sinusoid to extract the Gilbert damping parameter.

87 e first show how the increase of the Gilbert damping, caused by the inclusion rare-earth dopants such

88 aused by the Pinatubo 1991 eruption may have damped the observed decreasing trend of the AMOC in the

89 n the magnetically ordered phase and heavily damped electromagnons in the paramagnetic phase of LiCrO

90 s likely to cause phonon modes to be heavily damped and localized.

91 rporating a catalytically active but heavily damped metal, Pd, sustain multiple size-dependent locali

92 However, the heavily damped plasmon resonances of many catalytically active m

93 single-crystalline nanowires exhibit a high damping merit index, suggesting that crystalline nanowir

94 t a unique combination of stiffness and high damping capacity (60-70%), the latter exceeding that of

95 Numerical simulations in the high damping 'quasi-static' and low damping 'dynamic' regimes

96 Because the high damping of the material removes all other linear, small-

97 Light pulses caused intense and highly damped mechanical responses followed by traveling waves

98 filaments to result in cell death; however, damping of the enzyme activity induces the formation 3D

99 nificant extents of the magneto-hydrodynamic damping (MHD)-dependent solute build-up at the interface

100 ecruitment of cell types; and (iii) 10-20 Hz damped oscillations across retinal layers.

101 RE), with shear stiffness measured at 60 Hz, damping ratio at 40 Hz, and magnetic resonance imaging p

102 mice implicates a cholesterol derivative in damping down the inflammatory response mediated by inter

103 location rates can underlie the diversity in damping characteristics of calcium oscillations among ce

104 brissa that includes the effects of inertia, damping, and collisions.

105 tion, is dominated by the enhanced intrinsic damping contribution as a function of the Pt capping lay

106 his exceptional combination of low intrinsic damping and substantial magnetostriction arises from the

107 0.0036 +/- 0.0003 at 310 K for the intrinsic damping parameter.

108 a short-wavelength ion acoustic mode that is damped by electrons and reexcites small-scale Langmuir w

109 needs of harvesters, even if variability is damped in the archaeological record.

110 Its damping effects were confirmed when applied externally.

111 onlocality, electronic spill-out, and Landau damping.

112 This suggests that electron Landau damping could play a significant role in turbulent plasm

113 resonance shifts and surface-enabled Landau damping-a nonlocal damping effect-which have a dramatic

114 see text] and by linear phase mixing (Landau damping) when [Formula: see text].

115 [Formula: see text] The extinction of Landau damping enhances spatial optical coherence.

116 under conditions conducive to strong Landau damping.

117 Our results show that Landau damping is the dominant physical mechanism of hot-carrie

118 aster mixing, which is similar to the Landau damping in plasma physics.

119 asurements are rarely observed due to Landau damping by the single-particle continua.

120 This rapid mixing underlies Landau damping of these fluctuations in a quiescent plasma-one

121 lectron and hole carriers excited via Landau damping (during the plasmon decay) are responsible for t

122 lly: rather than being a system where Landau damping plays the role of dissipation, a collisionless p

123 eature an interesting regime in which Landau damping (dissipation via electron-hole pair excitation)

124 ity shows a signature consistent with Landau damping.

125 achieved by elastic metamaterials with large damping.

126 metallic ferromagnets generally have larger damping due to magnon scattering by conduction electrons

127 Responses in various forms like damped harmonic oscillation and periodic oscillation are

128 multimode optomechanical system, where a low damping mechanical mode in the unresolved-sideband regim

129 s in the high damping 'quasi-static' and low damping 'dynamic' regimes are compared and show clear di

130 This record low damping for metallic ferromagnets offers new opportuniti

131 ugh all of these great prospects require low damping, thus far strong plasmon damping has been observ

132 s ultrastrong field confinement and very low damping, enabling new classes of devices for deep-subwav

133 Low-damping magnetic materials have been widely used in micr

134 scillations.Owing to their conductivity, low-damping metallic ferromagnets are preferred to insulatin

135 into the origins of chiral magnetism in low-damping magnetic oxides and identify paths toward engine

136 Meanwhile, low-damping metallic ferromagnets are desired for charge-bas

137 So far, the lack of low-damping, magnetostrictive ferrite films has hindered the

138 This can be explained in terms of a lower damping of Fano resonance on obliquely deposited sample

139 s magnons, have low energy loss and magnetic damping, which are critical for devices based on spin-wa

140 tion, zero magnetic moment, and low magnetic damping can be achieved at the same time.

141 ; x ~ 2] has shown an extremely low magnetic damping comparable to, for example, yttrium iron garnet

142 Here the authors achieve low magnetic damping in CoFe epitaxial films which is comparable to c

143 devices, but it also has the lowest magnetic damping of any known material.

144 f a ferromagnet can act as negative magnetic damping and thereby excite self-oscillations of its magn

145 Hall angles even with moderate magnetisation damping values.

146 The intrinsic zero-temperature magnon damping in quantum spin systems can be driven by the int

147 The main damping channels are attributed to intrinsic thermal pho

148 ectable necroinflammation and fibrosis (mean damping ratio at 80 Hz and 20-week feeding, 0.044 +/- 0.

149 Additionally, using the measured damping rate of a levitated nanoparticle at a given pres

150 erials are being investigated for mechanical damping applications.

151 th, good superelasticity and high mechanical damping, and remarkable functional properties of high el

152 ustic measurements of the magneto-mechanical damping by domain walls.

153 oduced to model the observed opto-mechanical damping.

154 optical resonance-coined as opto-mechanical damping.

155 to giant enhancement of both the mechanical damping and the spring stiffness, facilitating low-power

156 inflammation through promoting IgG1-mediated damping of the FcepsilonRI-dependent acute-phase reactio

157 ion precession was fitted with a single-mode damped sinusoid to extract the Gilbert damping parameter

158 k shows that the power gain, or the negative damping, diminishes with intensity, we show explicitly b

159 activity are at marginal stability, neither damped (stable) nor exponentially growing (unstable) but

160 ymmetric line shape that suggests weak or no damping of the plasmon by ionized impurities.

161 ystemic relevance, imperfections like noise, damping, and trending, or limited sampling density.

162 In particular, nonlinear damping prevents excitation of coherent magnetization au

163 nd experimentally demonstrate that nonlinear damping can be controlled by the ellipticity of magnetiz

164 amental nonlinear phenomena is the nonlinear damping enhancement, which imposes strict limitations on

165 nd surface-enabled Landau damping-a nonlocal damping effect-which have a dramatic impact on the ampli

166 ter part of the oscillation that is normally damped; when this enhancement crosses perceptual thresho

167 The plasmon frequencies that are not damped by single-particle excitations do reach the near-

168 find a surface plasmon-polariton that is not damped by particle-hole excitations or the bulk modes an

169 Under optimum conditions (pH = 2; amount of damped MHAMS-MIONPs = 90 mg; eluent solvent volume = 2.6

170 In the absence of damping and driving, the mechanical model produces axial

171 larly magnetized materials in the absence of damping.

172 The effect of damping on the asymmetric wave transmission is further d

173 g in granular materials and the interplay of damping, weakening and inertial effects in bulk metallic

174 nd describe a novel and modulatable means of damping neuronal excitability.

175 peaks may have contributed to saturation of damping effects via nonlinear particle trapping.

176 attention, and there is little consensus on damping models.

177 Instead mosquitoes rely on damping by deforming two forelimbs and buckling of the p

178 Exposure to moldy or damp indoor environments is associated with allergic dis

179 esponse, it is revealed that the oscillation damping originates from the fluid viscosity while the os

180 e of the system exhibits purely oscillatory, damped oscillatory or monotic behaviour under certain pa

181 The over-damped relaxation of elastic networks constructed by con

182 the background signal, while only partially damping the signal in the presence of a catalyst.

183 Lyman alpha emission line (the Gunn-Peterson damping wing), as would be expected if a significant amo

184 finite energy, changing the anomalous phonon damping into an anomaly in the dispersion.

185 or-the eye muscles themselves-where physical damping of the oscillation offers an alternative approac

186 tes rather than seconds due to physiological damping of the released mechanical energy, thus protecti

187 We determine the dispersion and plasmon damping in real space.

188 We find unprecedentedly low plasmon damping combined with strong field confinement and confi

189 on and in-depth understanding of low plasmon damping is the key to the development of graphene nanoph

190 show that a substantial reduction of plasmon damping can be achieved by placing a nanometric polymer

191 require low damping, thus far strong plasmon damping has been observed, with both impurity scattering

192 al gate below the graphene, and that plasmon damping at positive carrier densities is dominated by Co

193 ptanal 'fatty cake crust', methional 'potato damp', and 2,5-dimethylpyrazine 'cake crust, nutty'.

194 ive rise to an effective trapping potential, damping, and attractive boson-boson interactions mediate

195 Magnetization relaxation, precession, damping and the spatial coherence of magnetization dynam

196 tection of germinating crops against Pythium damping-off disease.

197 re attributed to reduction in both radiation damping and resistive heating effects in the NWs.

198 bes due to broadening effects from radiation damping.

199 sults is suppressing the effect of radiation damping in (1)H NMR which produces signal distortion and

200 city, the wave fluxes of heat, and radiative damping.

201 e attributed to changes in the non-radiative damping and energy transfer.

202 ack of the first kind involves the radiative damping of the vertically uniform temperature perturbati

203 he dissipative nature of the polymer readily damps linear waves, preventing propagation of any mechan

204 hat a translocation embedded motif regulates damping of G-protein-mediated calcium oscillations consi

205 The remarkable damping performance of the hierarchically structured fib

206 nder diel conditions; however, these rhythms damped within 2-3 days after transfer to constant light.

207 erve that SOC significantly enhances the SDM damping while reducing the thermalization (the reduction

208 hat photonic sintering is an inherently self-damping process, i.e., the progress of densification red

209 ern level in the early Holocene and severely damped ~4000 to 5000 years ago.

210 may affect enzyme action due to significant damping in the enzyme fluctuations.

211 While the implications of spin damping for relaxation processes are intensively studied

212 , and how the action of the peripheral stalk damps the side-to-side rocking motions that occur in the

213 inaccessible combinations of high stiffness, damping and light weight that we achieve in these layer-

214 structure, in which we demonstrate a strong damping-like torque from the spin Hall effect and unmeas

215 his range inter-sub-band phonons show strong damping due to resonant scattering into an intermediate

216 which occur with high yield despite strongly damped and noisy environments.

217 tips, in which the gold plasmon was strongly damped by cadmium selenide through interfacial electron

218 lter on variations in magma supply, strongly damping fluctuations shorter than about 100,000 years.

219 elaxation processes are intensively studied, damping effects during impulsive spin excitations are as

220 computed dispersion relation leading to such damping was consistent with proposed continuum viscoelas

221 identified, namely bulk damping and surface damping.

222 as the temperature decreases, while surface damping shows an enhancement peak at the temperature of

223 eptional synthetic materials with tailorable damping behavior.

224 y time scales suggests additional short-term damping of solute concentrations, potentially due to in-

225 ncert with other hypothesized processes that damp dynamic ruptures, and is consistent with the broad

226 scence rhythms with periods of ~21-31 h that damped within ~3-4 days under constant light.

227 e of these persisting motions indicates that damping and intermode coupling are weaker than previousl

228 ry multistable dynamical systems such as the damped driven pendulum, a model of Amazonian rainforest

229 e of dielectric behavior is explained by the damped harmonic oscillator model with temperature depend

230 In the damped phase, the magnitude of the order parameter appro

231 ization in the strong coupling regime to the damped-dynamics in the weak coupling regime, is a signat

232 Using the damped resonance, we demonstrate three types of broadban

233 The damping of the microbunching instability, through the us

234 changes in the reorganization energy and the damping factor of the molecular bridges, in addition to

235 tion of the perpendicular field-like and the damping-like SOTs, which exhibits deterministic switchin

236 the perpendicular field-like torque and the damping-like torque coexist, hence jointly affecting the

237 rigin of fluidic HU can be understood as the damping of a stochastic harmonic oscillator in q space,

238 ption effect is characterized further by the damping frequency of the relaxation mode and the decay r

239 nticipate and quantify the anisotropy in the damping behavior with respect to curvature.

240 role of hyperbolic surface scattering in the damping process of hyperbolic phonon polaritons.

241 hotoacoustic spectroscopy to investigate the damping of a single sub-terahertz coherent phonon mode b

242 ar modulus output generated by mf3D-MRE, the damping ratio at 40 Hz and shear stiffness at 60 Hz best

243 ficance of the relative contributions of the damping and the IDMI from the heavy metal layer on the m

244 A systematic study of the damping parameter and frequency as a function of irradia

245 g effects, thereby enabling tailoring of the damping processes and electromagnetic field couplings of

246 ng that originates from the variation of the damping rate and coupling coefficient of the resonance m

247 oriya interaction (IDMI), enhancement of the damping, via d-d hybridisation and spin-pumping across t

248 It is demonstrated that the role of the damping-like SOT in the deterministic switching is highl

249 ain-wall velocities depend critically on the damping rate.

250 dically driven optical cavity can reduce the damping of a mechanical resonator, leading to parametric

251 rate of a signaling protein can regulate the damping of system oscillation.

252 deling framework that naturally stylizes the damping effect of borders.

253 Importantly, our theory reveals that the damping dissipation and active reciprocal interaction (d

254 Next, we show that the damping rate of cultured cells can be changed in a dose-

255 In this study, we show that the damping rate of population-level bioluminescence recordi

256 It is shown that the damping within the resonators determines the trade-off b

257 colloids are usually disregarded due to the damping imposed by the surrounding fluid.

258 the domain wall velocity behaviour when the damping is larger.

259 no bulk pair breaking takes place, while the damping observed originates from the bound states coveri

260 ent becomes more important compared with the damping and coupling effects from the normal component.

261 Compared with the damping of the homogeneous composition FeNi nanowire (a

262 mputing and signal processing, because their damping can be lower than the ohmic losses in convention

263 mulative oceanic heat loss from ENSO thermal damping reduces stratification of the upper equatorial P

264 The associated atmospheric nonlinear thermal damping cools the equatorial Pacific during El Nino but

265 disks are mostly free of bulk thermoelastic damping.

266 ic phonon scattering limits or thermoelastic damping limits.

267 This damping of diversification rates indicates ecological li

268 lung volume, static lung compliance, tissue damping, and tissue elastance).

269 y redistribution caused by the OWBCs acts to damp the near-surface atmospheric baroclinicity and comp

270 e proposed mechanism employed by the body to damp the impact is through vibrations of the skeletal mu

271 The enhanced ability of MT bundles to damp buckling waves relative to individual MT filaments,

272 ovel role for cMyBP-C N'-terminal domains to damp sarcomere-driven contractile waves (so-called spont

273 Exposure to damp indoor environments is associated with increased ri

274 rth magnet oculomotor prosthesis, powered to damp nystagmus without interfering with the larger force

275 e globe, action at a distance is required to damp the oscillation at the point of fixation, allowing

276 r interventions, it is shown successfully to damp pathologic eye oscillations while allowing normal s

277 fluxes on the equatorward side would tend to damp the SST front, here we present observational eviden

278 shape-agnostic manner and with resistance to damping.

279 es including stiffness, strength, toughness, damping, fatigue resistance, and self-healing ability is

280 show that, unlike in ferromagnets, ultrafast damping plays a crucial role in antiferromagnets because

281 esolved measurements, we find that ultrafast damping results in an immediate spin canting along the s

282 e system approaches equilibrium it undergoes damped oscillations with a ~3.6-picosecond time period.

283 bly increases optical losses through various damping channels.

284 echanism to design oscillations with varying damping patterns by using intracellular translocation of

285 can be mitigated by increasing ventilation, damp cloth cleaning, and minimizing the use of phthalate

286 nt masses which interact with each other via damped translational and torsional springs, and with the

287 equency of the vibration plate and vibration damping beyond the resonance.

288 res below ~ 100 K, C(60) lattice vibrational damping is mitigated and the quantum dynamics of confine

289 theory (MKT), the influences of both viscous damping and solid-liquid retarding were analyzed in eval

290 that biomimetic scale beams exhibit viscous damping behavior even when only Coulomb friction is post

291 ing limitations, and the increase in viscous damping at low Reynolds numbers.

292 dissipation that originates from the viscous damping of the dithered cantilever.

293 ation and lump the viscous effect to viscous damping components.

294 eptide or its receptor, mCry1 expression was damped and desynchronized between cells.

295 erfluid component via mutual friction, which damps the motion of quantized vortex lines and eventuall

296 to lower the allergen burden associated with damp homes.

297 y an undamped elastic element in-series with damped elastic elements, adapts its length to the SL wit

298 length of the acceptor is investigated, with damping coefficients beta measured to be (0.24 +/- 0.025

299 a Gilbert type at the saturated state, with damping of 0.035 +/- 0.003.

300 er suppression and anomalous cooling without damping in an asymmetrically-pumped optomechanical syste