ライフサイエンスコーパス: finite

1 The stiffness of that interface is finite.

2 The local moment per Ru site remains finite 2.3 mu B in the whole temperature range investig

3 strained and controlled by the addition of a finite acid concentration to the system.

4 ory theory, which analyses the allocation of finite amounts of energy between four competing function

5 Effect of finite and infinite sample volume conditions, as well as

6 s the rich behavior of amplification in both finite and infinite spin environments, from quadratic gr

7 rily because the observable data are sparse, finite and noisy.

8 are now gaining traction as models of scale-finite animal movement patterns because they overcome in

9 ere, we describe how plasmonic superlattices-finite-arrays of nanoparticles (patches) grouped into mi

10 ry conditions typical for batch experiments (finite bath), desorption accelerates with increasing par

11 eduction as a result of the depletion of the finite bioavailable Fe(III) pool.

12 ravenous iron administration associates with finite but important risks.

13 ch as ethene-like C2O4(4-) in C2/m Li2(CO2), finite C4O8(6-) chains in P1 Li3(CO2)2, one-dimensional

14 ties include various types of architectures: finite cages or shells, essentially unbounded two-dimens

15 urothelium maintained in organ culture or as finite cell lines in vitro.

16 ulations of neurons, which are inevitable at finite cellular concentrations, are likely to be the mai

17 ination states localized at the edges of the finite chain resulting in localized lasing and dissipati

18 ing heats of transport of individual ions at finite concentration remains an outstanding question bot

19 e heats of transport of aqueous solutions at finite concentrations, and apply our method to study lit

20 vealing that (in such a many-body resonance) finite conduction is achieved from a charge frozen by Co

21 ave experienced a complex environment with a finite correlation time.

22 itonic component of the polariton provides a finite Coulomb scattering cross section, such that the d

23 WS2 /MoS2 semiconducting heterobilayers and finite density of states of graphene electrodes.

24 We define a finite developmental window for motile cilia in zebrafis

25 Finite difference analysis of ion-selective membranes is

26 Finite difference coefficients are then computed by mini

27 two well-separated bodies at temperatures of finite difference in vacuum.

28 diffusion model in both a 3-dimensional (3D) finite difference method and a 2-dimensional (2D) level

29 e and sample solution phases by means of the finite difference method.

30 ate that this method is superior to standard finite difference methods, while comparable to Zhang's o

31 y this phenomenon and were evaluated using a finite difference model developed to simulate the adsorp

32 nsity profiles is achieved on the basis of a finite difference model, with excellent agreement betwee

33 al derivatives of the mapped wavelet and the finite difference operator over all propagation angles.

34 d is capable to maximise the accuracy of the finite difference operator.

35 thods, while comparable to Zhang's optimised finite difference scheme.

36 The resulting finite difference simulation is much more robust than th

37 ie aperture is numerically modeled using the Finite Difference Time Domain (FDTD) method.

38 are found to be in excellent agreement with finite difference time domain (FDTD) simulations.

39 f linear, isotropic materials, it utilizes a finite-difference method on a staggered grid to solve fo

40 s of SPR under plane-wave illumination and a finite-difference time-domain (FDTD) simulation was used

41 Experiments and finite-difference time-domain (FDTD) simulations demonst

42 Both experiments and finite-difference time-domain (FDTD) simulations show th

43 distribution of the waveguide calculated by finite-difference time-domain simulations, suggesting th

44 A three dimensional finite-difference-time-domain (FDTD) simulation has been

45 for a stress tensor accurate to first-order finite differences and motivates the use of distance-bas

46 k content and work of formation of arbitrary finite dimensional quantum states when the fluctuations

47 ary conditions are applied to the fluid at a finite distance above the ciliated edge.

48 arizable nanostructures over a wide range of finite distances can only be attained by accounting for

49 cement, and the other consists of genes with finite, distributed replacement rates.

50 its a T (2) dependence, which shows that for finite doping a Fermi liquid state survives-however, wit

51 or determining which patients should receive finite-duration NUC therapy and which should receive com

52 ombining musculoskeletal (MS) modelling with finite element (FE) analysis.

53 ding molecular dynamics (MD) simulations and finite element (FE) modelling.

54 correspondence principle was validated using finite element (FE) simulations and by comparison with t

55 Finite element analysis (FEA) simulations demonstrate th

56 trabecula segmentation (ITS)-based analysis, finite element analysis (FEA), energy dispersive X-ray s

57 ll with the simulation results obtained from finite element analysis (FEA).

58 em to facilitate the analysis of AAA using a finite element analysis based approach.

59 Finite element analysis confirms that this effect is due

60 Purpose To describe a nonlinear finite element analysis method by using magnetic resonan

61 A nonlinear finite element analysis method was developed to estimate

62 lusion This experiment demonstrates that the finite element analysis model can consistently and relia

63 A complete 3-dimensional (3D) finite element analysis model of a minimally reduced mol

64 This provides a target for finite element analysis of the flow of silk proteins, wi

65 system was first considered by conducting a finite element analysis simulation, and then a demonstra

66 images by using phantomless calibration and finite element analysis to measure bone mineral density

67 A MRI-based finite element analysis was generated to characterize th

68 ography, and bone strength with the use of a finite element analysis, and we evaluated dietary protei

69 ation of computational biomechanical models (Finite Element Analysis, Multibody Dynamics Analysis) de

70 related mechanics is further rationalized by finite element analysis, the generalized shear-lag theor

71 ice designs through theoretical modeling and finite element analysis.

72 To address this question, we developed a new finite element approach to model diffusion on curved mem

73 These data are used in numerical finite element calculations in hydrothermal pores for va

74 sured, and the results are compared with the finite element calculations.

75 -1,6-dichlorohexane interfaces together with finite element computational simulations.

76 ng 4-D light sheet imaging with a stabilized finite element flow solver, and extract time-dependent m

77 Using a new one-dimensional porous medium finite element gas-exchange model parameterized with lig

78 vanced Multiphysics modelling software (e.g. Finite Element Method (FEM) etc.) and home-made develope

79 Comprehensive finite element method (FEM) modeling has been undertaken

80 Finite element method (FEM) modeling places the techniqu

81 astoplastic material under high pressures in finite element method (FEM) simulations.

82 mulation and experimental verification using finite element method and fabricated structures made fro

83 perimental studies are supported by detailed finite element method modeling that places the technique

84 Finite element method simulations confirm that the hydro

85 Finite element method simulations elucidate the governin

86 iments, transmission electron microscopy and finite element method simulations to fully characterize

87 , we adopt an electromagnetic model with the finite element method to elucidate cooperative chirality

88 ass-transport conditions and analyzed by the finite element method to kinetically resolve all steps o

89 al simulations have been carried out via the finite element method to propose the underlying working

90 thoroughly assess the reproducibility of the finite element method, three separate analyses were perf

91 al analyses by cellular force microscopy and finite element method-based modeling revealed significan

92 stics using quasi-mode analyses based on the finite element method.

93 l observations, and demonstrate the value of finite element methods at the continuum level for design

94 piecewise continuous mesh used to develop a finite element model in two dimensions.

95 Furthermore, a 3-dimensional finite element model of a cell on a vibrating substrate

96 nscranial electrical stimulation including a finite element model of brain current flow, numerical si

97 In this paper, we present a robust finite element model that provides a deep understanding

98 f a kinematical model, a fully deformable 3D finite element model was used.

99 Using a finite element model, we characterize the dynamics of so

100 [CT]) and that of a numerical analysis with finite element modeling (FEM) in the prediction of failu

101 Finite element modeling indicates that the size and thic

102 The results of detailed experiments and finite element modeling of metal micro-droplet motion as

103 Finite element modeling supports the experimental observ

104 l-atom molecular dynamics and coarse-grained finite element modeling to DX-based nanoparticles to elu

105 We use embryonic tissue explants, finite element modeling, and 3D cell-patterning techniqu

106 Finite element modeling, mechanical testing, and immunoh

107 r, we provide a new numerical model based on finite element modeling.

108 u neutron diffraction and crystal plasticity finite element modeling.

109 This investigation presents finite element models of the eye lens based on data from

110 l stimuli parameters we develop 3D nonlinear finite element models.

111 A three-dimensional finite element numerical modeling for the scanning micro

112 In this study, we generated and analysed 31 Finite Element planar models of different primate jaws u

113 tum corneum is obtained using the commercial finite element program COMSOL Multiphysics.

114 The finite element simulation of sphere-cap ITIES tips accou

115 o match with numerical solutions obtained by finite element simulation of unsteady fully coupled Pois

116 Finite element simulation reveals that the anomalously h

117 A finite element simulation reveals that the developed met

118 Via 3-d finite element simulation studies, we demonstrate direct

119 of multiple fiber bundles, three-dimensional finite element simulations are conducted.

120 gh an inverse identification method in which finite element simulations are fitted to the experimenta

121 Finite element simulations determined that pin displacem

122 Finite element simulations show that the failure is gove

123 Results from finite element simulations showed good agreement with th

124 train localization and the free-volume-based finite element simulations that predict the evolution of

125 method is described by Nernst-Planck-Poisson finite element simulations, and both amperometric and po

126 Using finite element simulations, we establish a new protocol

127 ere-cap UMEs and corroborated with data from finite element simulations.

128 acoustic phonon modes, which are compared to finite element simulations.

129 nt monitoring method and numerically through finite element simulations.

130 solutions are applied for validations of the finite element solutions.

131 brant-loaded extraction phase, CL-EP, with a finite-element analysis (FEA) using COMSOL Multiphysics

132 ing X-ray computed tomography, and performed finite-element analysis of the mechanical response withi

133 and validated by experiments and means of a finite-element model.

134 ng nanoindentation, acoustic microscopy, and finite-element modeling for probing the tooth's mechanic

135 Finite-element modeling projected myofiber stress reduct

136 Finite-element modeling suggests that the absorption of

137 in the naturally feasible design space using finite-element modelling and found that design affects e

138 Finite-element modelling of the stress distribution with

139 eric density model of the region; subsequent finite-element modelling shows that seismicity focuses i

140 Our three-dimensional viscoelastic finite-element models of the post-earthquake deformation

141 To address this paradox we develop finite-element models subjected to extensional and gravi

142 To deduce the current density distribution, finite-element models were constructed on the basis of t

143 Using finite-element models, supported by analytical methods,

144 odel is based on a hybrid cellular Potts and finite-element simulation framework describing a mechani

145 ed by controlled debonding in agreement with finite-element simulation results.

146 rade of precision of our application we used finite-element simulations to investigate how the concen

147 Crystal-plasticity finite-element simulations were employed to qualitativel

148 when coupled with modeling predictions from finite-element simulations.

149 turing methods, and inform our designs using finite-element simulations.

150 al-element time-domain method (SETD) and the finite-element time-domain (FETD) method.

151 Molecular dynamics and finite elements simulations are used to gain further und

152 Biological objects, however, have finite extent and offer different topologies, such as th

153 1 was characterized by rapid reduction of a finite Fe(III) pool along the edges of the clay particle

154 es the limit imposed by diffraction from the finite field extent in the grating region.

155 ed algorithm to correct the measurements for finite filament length as well as photobleaching.

156 for every [Formula: see text] there exists a finite [Formula: see text] so that the observer obtains

157 The particle-hole symmetry occurs around a finite frequency, and hence we can witness a dynamical t

158 In response to severing, a finite gap forms and is repaired by recruitment of new m

159 r of states as required for the traditional (finite) HMM.

160 utomorphisms has a translational subgroup of finite index acting freely on the structure.

161 er, the true dynamics of angular momentum in finite, interacting many-body systems like trapped Bose-

162 ted this anomalous domain periodicity to the finite lateral-size effect of a ferroelectric nanodot wi

163 that treats the neutrons as wave packets of finite length and the protein as a random walker in the

164 ) in order to avoid complications due to the finite length of time needed detect heat flow in the cal

165 with each round of cell division, placing a finite limit on cell growth.

166 domain, where one of the boundary walls has finite mass and is attached to a linear spring.

167 Finite mate search rate triggers Allee effects in our mo

168 We address the control of finite measures of criticality using data on fight sizes

169 long-term instability can be limited by the finite memory between these elementary features.

170 ory, while a quantum simulator requires only finite memory.

171 tistate mark-recapture methods to estimate a finite mixture model accounting for UH in all vital rate

172 Occupancy models incorporating a finite mixture model on detection - a new extension to c

173 Finite mixture modeling can be applied to serological da

174 can be estimated from serological data using finite mixture modeling.

175 Finite mixture models were used to identify the number o

176 phate rock, the source of P fertilizer, is a finite natural resource, there is a need to enhance P fe

177 A classification (finite number of classes) and a regression (continuous m

178 RNAi in worms, which typically persist for a finite number of generations.

179 , limits in drift due to steep gradients and finite number of receptor-methylation sites for adaptati

180 : define a cost function given by a sum of a finite number of replicas of the original cost function,

181 cannot reach absolute zero temperature in a finite number of steps and within a finite time.

182 ross-react with multiple antigens allows the finite number of T cells within an organism to respond t

183 heat engine which uses a small system with a finite number of ultracold atoms as its working substanc

184 p in which no eigenvalue exists as well as a finite number of zero eigenvalues.

185 n individual cell involves reactions between finite numbers of molecules, and this can result in inhe

186 tend with intrinsic noise that arises due to finite numbers of proteins.

187 s in most vertebrates are unidirectional and finite once the individual reaches full size [1].

188 n number 2 and intrapocket paired state with finite pair momentum.

189 cer returning for follow-up and may define a finite period of increased risk after diagnosis.

190 In this paper a practical case of a finite periodic Parity Time chain made of resonant diele

191 The band-structure of the finite periodic PT resonator chains is compared to infin

192 By activating Src for finite periods of time, we reveal how the duration of ki

193 le chains, for semi-flexible polymers with a finite persistence length [Formula: see text] the trans

194 increase of wall shear stress from zero to a finite physiologically relevant value.

195 le relationship on a rapidly urbanizing, yet finite planet.

196 re we show that the collective activity of a finite population of bistable units (i.e., a generalized

197 mics would be reproduced quantitatively by a finite population of distinct neural assemblies, each wi

198 ultiple phenotypic states, introduced into a finite population of individuals that can express only a

199 tionary dynamic of cyclic dominance within a finite population.

200 udy stochastic evolutionary game dynamics in finite populations to systematically compare the evoluti

201 ifference to mutation-selection processes in finite populations.

202 enario for the evolution of recombination in finite populations: the genomic storage effect due to ph

203 orcement learning as a stochastic process in finite 'populations of ideas'.

204 dissimilar nanorods separated by a thin but finite potential barrier and theoretically derive the fr

205 In the case of finite PT-chains, and for a particular type of modulatio

206 e- and two-photon superposed states with the finite (quantised) number of peaks in the quantum regime

207 We consider a finite, randomly mating population initiated from an inf

208 nsity correlation functions reveals a hidden finite-range antiferromagnetic order, a direct consequen

209 calculated by a Hubbard model with suitable finite-range interactions.

210 eading leads to exponential networks for any finite rate of infectiousness when the disease persists.

211 However, at a finite rate, TG2 transitions to an open conformation tha

212 In anoxic solution, CdTe dissolved at a finite rate.

213 An extended sink model, incorporating a finite reaction zone, was able to fit all data satisfact

214 Cot excess under temperature conditions of a finite residence time of the molecule, the reactand diff

215 ions, the role of the constraints imposed by finite resource supply, and a comprehensive empirical ve

216 Allocation of finite resources to separate reproductive functions is p

217 In the face of finite resources, allocations of research and health-car

218 a widely accepted approximation to the exact finite sample conditional inference.

219 We show that for finite sample sizes with increasing number of null predi

220 ic categories that remain unrepresented in a finite sample.

221 symmetry breaking and take into account the finite sampling issue by introducing a tolerance paramet

222 ale magnetic resonance probes, for instance, finite sampling times greatly limit the achievable sensi

223 After removing the noise caused by finite sampling, we show that the similarity of an unkno

224 es is hindered in the ultrathin limit by the finite screening length of surface charges at metal-insu

225 lation of multiple biological processes by a finite set of transcription factors (TFs).

226 t of a single fibre core is dominated by the finite signal-to-noise ratio (SNR) afforded by current s

227 Finite simple groups are the building blocks of finite s

228 metastatic tumors suggests that employing a finite-sites model leads to improved inference of tumor

229 om noisy single-cell sequencing data under a finite-sites model.

230 evelopment of inference methods that utilize finite-sites models.

231 The effect of finite size and strain relaxation on the magnetic domain

232 bsence of coherent strain between Pt and Pd, finite size effects introduce local compressive strain,

233 sure isobars exhibit sloping plateaus due to finite size effects on reaction thermodynamics.

234 e examine a contraction mechanism based on a finite size of myosin clusters and anisotropy of force g

235 down in the Kohn anomaly associated with the finite size of the remaining graphene sites surrounded b

236 o uncover the thermodynamic laws that govern finite size systems which may in addition host quantum e

237 to the discovery of a set of second laws for finite size systems.

238 urprisingly, cell collectives, despite their finite size, show features of criticality known from pha

239 g into account fluctuations and the system's finite size.

240 ve Coulomb blockade transition, which is the finite-size analogue of the interaction-driven Mott meta

241 We use a finite-size analysis method to identify the type of phas

242 m be extrapolated by analyzing a sequence of finite-size cases?

243 he quantum critical point of the transition, finite-size effects lead to a nonzero gap.

244 e expression of heat capacity which includes finite-size effects, the work output is optimized with r

245 distribution among the individual layers of finite-size FLG systems using a novel spatial discrete m

246 Here, we study nonlinear properties of finite-size multimode -symmetric couplers and predict th

247 greatly enhancing the final QDS rate in the finite-size scenario.

248 pe systems of PDEs - which provides explicit finite-size solutions, matching recently investigated ph

249 enable the rational design and production of finite-sized anisotropic structures on the mesoscale.

250 ze, has been used to explain measurements of finite-sized droplets.

251 th high power densities (>5 W/m(2)) and with finite-sized heat exchangers.

252 ck of the skyrmion topological protection in finite-sized magnetic systems.

253 Chiral twist promotes the formation of finite-sized rafts and mediates a repulsion that distrib

254 n occur in interfacial Dzyaloshinskii-Moriya finite-sized systems.

255 ability distribution of the spin overlap for finite sizes.

256 similar scaling law can be obtained for the finite-speed quench as well within the Kibble-Zurek mech

257 While approximations that use finite-state machines (Pair HMMs and transducers) curren

258 We use a finite-state transducer where the emitted read depth is

259 he cardiac cycle was quantified by computing finite strain fields.

260 nlinear flow of a glass under deformation at finite strain rate.

261 Combining longitudinal MR imaging and finite strain theory, this study aimed to provide new in

262 often derived from the consideration of the finite-strain energy or the interatomic potential.

263 latory metabolite-enzyme interactions, but a finite structural diversity prevalent within the metabol

264 ompute on distributions that is complete for finite support distributions, and can be compiled to a r

265 om some desired target distribution that has finite support in [Formula: see text], with [Formula: se

266 variability in behavior among the agents in finite swarms with both alignment and cohesive interacti

267 ite simple groups are the building blocks of finite symmetry.

268 chord length, and have studied the effect of finite system size and porosity on such characteristics.

269 ain the trivial-to-topological transition in finite systems and to quantify the scaling of topologica

270 tigate the miscible-immiscible transition at finite temperature by means of Quantum Monte Carlo.

271 f tunnel current fluctuations, incorporating finite temperature contribution through consideration of

272 We consider finite temperature effects in a non-standard Bose-Hubbar

273 maximum value: [Formula: see text] Although finite temperature equilibrium dynamics will not yield h

274 We show experimentally that finite temperature maximum entropy decoding can give sli

275 Finite temperature micromagnetic simulations were used t

276 uced by both minimum energy calculations and finite temperature Monte Carlo simulations of hard core-

277 We then employ finite temperature simulations to probe how this affects

278 However at finite temperature, it describes a distinct geometrical

279 e inconsistent with a diverging viscosity at finite temperature.

280 e of the crystal structure across the MIT at finite temperature.

281 we report the first attempt to evaluate the finite-temperature pseudo-binary phase diagram of the Ti

282 wo-dimensional isotropic Heisenberg model at finite temperatures by the Mermin-Wagner theorem.

283 Importantly, at finite temperatures, the process of folding is probabili

284 amples these materials magnetically order at finite temperatures, the scale of which may imply weak f

285 However, the finite temporal recording length of current techniques h

286 erence between G 2W/G and G W/W uncovers the finite thermal resistance induced by the graphene layer.

287 Structural completeness conditions of the finite-thickness counterparts to the two types are also

288 However, with finite time and resources as well as a growing understan

289 es interventions in a dynamic fashion over a finite time window via a restricted set of controllable

290 mputational dynamic models reach infinity in finite time, extending analysis and numerics beyond it b

291 ns, the crossing of infinity may persist for finite time, necessitating the introduction of buffer zo

292 ure in a finite number of steps and within a finite time.

293 a general method for sampling an ensemble of finite-time, nonequilibrium protocols biased toward a lo

294 This ratio (computed for finite times on very large, effectively infinite, system

295 present, all flow states exhibit stimulated, finite two-fold mode.

296 be an endomorphism of a separated scheme of finite type over k We show that for any [Formula: see te

297 nary form of contest competition that yields finite upper bounds on species richness.

298 lated drag reduction due to the formation of finite velocity at porous surfaces is still relatively u

299 eigenvalue distribution is found to follow a finite-width probability density function with certain s

300 age-like to nanograting modification after a finite writing length in a transparent dielectric is phe