ライフサイエンスコーパス: be described by

1 Combinatorial chromatin patterns were described by 42 major chromatin states with selecte

2 The four VS domains are described by a continuum electrostatic model under v

3 These charge-transfer chromophores are described by a D(1)-A-D-A-D(1) structure comprising

4 The electronic properties of graphene are described by a Dirac Hamiltonian with a four-fold sy

5 erial cytochrome c peroxidase (bCcP) enzymes are described by a homodimeric state.

6 The sequencing counts are described by a lognormal-beta-binomial hierarchical

7 proteins and the mechanical effects induced are described by a model based on spontaneous curvature

8 The effects of irradiation are described by a modified version of the linear-quadra

9 Our measurements are described by a new model where the Poisson ratio dri

10 Reaction kinetics are described by a rapid, low-fractionating uptake step

11 live cells indicates that these fluctuations are described by a single diffusion constant in log GFP

12 Bivalve, ammonite and snail shells are described by a small number of geometrical parameter

13 The in-plane depolarized fluorescence decays are described by a stretched exponential law.

14 nctions from smoking cessation interventions are described by a three-state Markov model.

15 h as the Type Iax-class prototype SN 2002cx, are described by a variety of models such as the failed

16 We find that peptoids can be described by a "rotamer" treatment, similar to that e

17 e dependence of fluorescence intensities can be described by a 15-state model of the transport cycle

18 ical, and the molecular spacing for both can be described by A = 1.42 +/- 0.02 nm, B = 1.32 +/- 0.02

19 luctuating stimuli is largely linear and can be described by a biphasic temporal filter and dynamical

20 At pressure <6 GPa, the PAW-GGA can be described by a Birch-Murnaghan equation of state with

21 t boundary diffusion in helical peptides can be described by a classical, Einstein-type, 1D diffusion

22 ial antimicrobial susceptibility may need to be described by a combination of parameters rather than

23 ned by a single cooperative pathway, but can be described by a competitive two-pathway mechanism.

24 The motion of these resonators can be described by a double-well potential with a large cen

25 that crystalline doxorubicin dissolution can be described by a first order rate constant of 1.0x10(-9

26 across different vegetation communities can be described by a Fourier model.

27 ic behavior of the solid-phase reactor could be described by a fractal Michaelis-Menten model with a

28 firmly established that protein folding can be described by a funneled energy landscape.

29 of structural formation was studied and can be described by a generalized model of nucleated polymer

30 This quantitative dependence can be described by a Hill equation, with a Hill coefficient

31 While the system can only be described by a large hierarchical set of equations in

32 easured for MBD3 bound to methylated DNA can be described by a linear combination of those for the me

33 he solvent-dependent aggregate stability can be described by a linear free-energy relationship.

34 urces and those predicted in models, and can be described by a mechanism suitable for implementation

35 Antibody responses in African children can be described by a model 15 including both short-lived AS

36 Globally, the datasets could be described by a monomer-dimer-tetramer-hexamer or a mo

37 Complex economic systems can often be described by a network, with nodes representing econo

38 pH 8 at both oxic and anoxic conditions can be described by a new model that incorporates Fe(II) rel

39 the intrinsically nonequilibrium system may be described by a non-Hermitian Hamiltonian.

40 dence suggests that cytoplasmic rheology can be described by a poroelastic model, in which the cytopl

41 quency clonotypes for which distribution can be described by a power law.

42 with HNO3/nitrate surface density and could be described by a simple analytical equation.

43 on of voltage-dependent K+ channels (Kv) can be described by a simple one-step occlusion mechanism, i

44 also find that the folding mechanism cannot be described by a simple two-state model, but rather is

45 s classical organellar proteomics and cannot be described by a single and ultimate list of protein co

46 mplex, where the Gcn4-Gal11 interface cannot be described by a single conformation.

47 Results show signals can be described by a single linear transition path with dif

48 tional changes, and show that F-actin cannot be described by a single molecular model.

49 The sampling and extraction of WSOC can be described by a single parameter, P, expressing the ra

50 lator transition in disordered systems could be described by a single parameter, the ratio of the ave

51 currently thought that filament kinetics can be described by a single rate constant for each end.

52 olution of gene blocks in proteobacteria can be described by a small set of events.

53 hanistic complexity of the linker region can be described by a spring model with Brownian motion of t

54 susceptible-infected-recovered mechanism can be described by a stochastic birth-death process of Galt

55 at photo-activated electron transport cannot be described by a superposition of the properties due to

56 ows weak net directional movement, which can be described by a thermodynamic sink arising from the di

57 These dynamics could be described by a three-state model involving stochastic

58 he presence of gene flow, a phylogeny cannot be described by a tree but is instead a directed acyclic

59 Overall, bacterial phenotypic evolution can be described by a two-stage process with a rapid initial

60 nding within the [W(mu-H)Si(mu-H)W] core can be described by a variety of resonance structures, some

61 The regulation of their activity has been described by a hierarchical model in which elements

62 iezoelectric fields associated with the SAWs being described by a relatively simple classical relaxat

63 ollected using cw laser excitation at 785 nm is described by a 300 K thermal distribution of excitati

64 that directional guidance along fibre tracts is described by a bimodal von Mises-Fisher distribution

65 ing that the two-dimensional electron system is described by a Bloch Hamiltonian, system is insulatin

66 between 100 mega-electron volts and 400 GeV is described by a broken power law that is statistically

67 am having multiple degrees of freedom (DoFs) is described by a coherency matrix G spanning these DoFs

68 The structure of materials is described by a combination of rotations, rotation-inv

69 The cellular phenotype is described by a complex network of molecular interacti

70 Mathematically, the model is described by a coupled system of reaction-diffusion e

71 opulations such that the demographic history is described by a deterministic nonlinear dynamical syst

72 e two strategies, A and B, whose interaction is described by a general payoff matrix.

73 strain-generated signaling molecule, and it is described by a kinetic multi-stage model.

74 rders of magnitude with Fe(II)/Fe(total) and is described by a linear free energy relationship.

75 tical framework in which a real-world system is described by a low-dimensional equation system with a

76 in the absence of magnetic anisotropy terms is described by a Mobius transformation in complex stere

77 istics observed in the native membranes, and is described by a multisquare model with Schiff base dep

78 tacts that are about to slide, whose density is described by a nontrivial exponent [Formula: see text

79 rection and magnitude of the resulting shift is described by a phase response curve (PRC).

80 light depends on the timing of exposure and is described by a phase response curve (PRC).

81 of cw (continuous wave) excitation intensity is described by a power law with exponents sequentially

82 we find that detachment of a suspension drop is described by a power law; specifically we find the ne

83 This antitumor immune response is described by a primary and a secondary (or memory) re

84 t of moving molecules in the porous particle is described by a random-walk.

85 Each entity (agent, lectin or ligand) is described by a range of properties that are summarize

86 A computer OS is described by a regulatory control network termed the

87 EVOO's) endogenous polyphenols; the reaction is described by a sigmoidal curve.

88 The factor is described by a simple linear combination of buried su

89 second-harmonic generation intensity, which is described by a simple model that accounts for the int

90 namics of the bending/straightening response is described by a single dimensionless "bending number"

91 From the theory point of view, this motif is described by a single gene regulation function based

92 version of the ferric and ferrous conformers is described by a single midpoint potential of -80 +/- 9

93 The acentric structure is described by a superposition of 168 atomic displaceme

94 an anisotropic magnetic susceptibility that is described by a tensor with a radially oriented princi

95 al strength upon pump and probe polarization is described by a theory of transient stimulated Raman s

96 tercalators, we find that ligand association is described by a two-step process, which consists of fa

97 a positive threshold Q in the inertial range is described by a universal q- exponential function, P(t

98 , the control of ion flow by the gate domain is described by a vapor-lock mechanism, and the simple c

99 Between treatment variability was described by a mixed effects model.

100 -transport code where the sorption of cesium was described by a multisite ion-exchange model.

101 Mucus velocity was described by a positive vector (toward the glottis)

102 lted in kinetic isotope fractionation, which was described by a Rayleigh model with an enrichment fac

103 The loss of vitamin D(3) during storage time was described by a second order reaction.

104 a ganglion cell's excitatory synaptic inputs were described by a divisive interaction between excitat

105 The results were described by a kinetic model allowing the simultane

106 e mobile segment of troponin-I to troponin-C were described by a simple kinetic scheme.

107 The surface pressure decay during depletion were described by a stretched exponential that suggested

108 showed that the displacements of these seals were described by a truncated power law distribution acr

109 The burden of illness can be described by addressing both incidence and illness se

110 gical management for acute anxiety and pain, are described by age and development.

111 butions of histopathology and polyp location were described by age and gender.

112 Although systems driven by small-step motors are described by an effective temperature and are thus q

113 Chemical reactions can be described by an energy diagram along a reaction coord

114 Other experiments could not be described by an equilibrium model, suggesting that a

115 e kinetics of cellulose hydrolysis have long been described by an initial fast hydrolysis rate, taper

116 nic ground state of the Au25(SC8H9)18(-) MPC is described by an eight-electron P-like superatom orbit

117 ed endosomes indicates that particle capture is described by an over-dispersed Poisson probability di

118 Muscle activations were described by ankle and hip EMG signals, with each E

119 nt numbers of human transcripts have not yet been described by annotation projects, while existing tr

120 nd anomalous supercurrent enhancement cannot be described by any known conventional phenomenon of Jos

121 istic states, massless Kane fermions, cannot be described by any other relativistic particles.

122 At large distances the heat transfer can be described by black body radiation, at shorter distanc

123 The excitations are described by Boltzmann distributions with their fact

124 ess cost C and the resistance ratio Rr could be described by C = 24.47/(1 + exp([1.57 - Log10Rr]/0.2)

125 under supersaturated water vapour conditions is described by classic Kohler theory.

126 eproducible electrochemical signals that can be described by classical electrochemical theory as well

127 etre dimensions exhibit features that cannot be described by classical electrodynamics.

128 hat the nucleation of amyloid fibrils cannot be described by classical nucleation theory: in the two-

129 nmental (plant leaves and sand) surfaces can be described by classical sorption isotherms.

130 Phage-sand interactions were described by colloidal filtration theory and the ex

131 Niche differences could only be described by combinations of traits, corresponding to

132 ults demonstrate that brain adaptability can be described by common processes that drive the dynamic

133 s: Dynamic electrochemistry in the gas phase is described by considering the ionized medium of a flam

134 The observed results were described by considering the potentials of redox pa

135 targets and functions of ubiquitylation have been described; by contrast, few targets of NEDD8 have b

136 ansport mechanism is not well understood and is described by controversial models.

137 nanodots toward the electroreduction of H2O2 was described by cyclic voltammetric and amperometric te

138 KCl is described by Debye-Huckel screening and a Manning con

139 und that these differences in processing can be described by defining a processing signal that is com

140 ii) a model where the communication topology is described by Delaunay triangulation, which is defined

141 between samples and ageing treatments could be described by differences in the water content and dis

142 hese two systems of behavioural control have been described by different learning algorithms, model-b

143 ater, the kinetics of unimolecular reactions are described by diffusion of a Brownian particle over a

144 lutes in nonreactive porous media can mostly be described by diffusion driven by the concentration gr

145 ic constants, the friction-load relationship was described by DMT mechanics.

146 all of our data together, the effects cannot be described by doping alone.

147 e, bottom-up control of phytoplankton cannot be described by either one alone, nor by a combined metr

148 and its response to environmental variation are described by empirically derived equations that repl

149 ic region of the dispersion the solitons can be described by envelope functions satisfying the nonlin

150 e protein structure while enzymatic function is described by Enzyme Commission numbers.

151 discover self-similar properties that cannot be described by existing models and discuss possible sce

152 The transient plasticity of period was described by existing mathematical models of the Ara

153 Atomic configurations were described by feature matrix based on internal vecto

154 al 180(o) commensurate magnetic domains, can be described by ferromagnetic and ferroelectric domains

155 Doxorubicin leakage can be described by first order rate constant for transport

156 he behavior of individual molecular formulas was described by fitting the single exponential model to

157 Without SP, the kinetics of Pi release are described by four phases: a "lag," a "burst" of ATP

158 Thus, dynein's motor functions can be described by four basic modes of motion: processive a

159 The CO2 emission reductions are described by g CO2/km emission targets for average n

160 models appear in TIGRFAMs, while 628 systems are described by Genome Properties.

161 re colony geometry and public good diffusion are described by graphs.

162 Treatment effects on PFS and OS were described by hazard ratios (HRs), median times to e

163 The unfolding of Pfk-2 induced by GdnHCl has been described by highly cooperative three-state equilib

164 We report several features that have not been described by in vitro analysis of the process, chie

165 consists of, the functional status of which is described by 'intestinal permeability'.

166 erobserver and intraobserver reproducibility were described by intraclass correlation coefficients (I

167 ider locomotion along a surface where forces are described by isotropic Coulomb friction.

168 observation times the dynamics can sometimes be described by isotropic random walks, usually the dire

169 the material's plastic properties, which can be described by its stress-strain behaviour.

170 getics of a protein's folding process, which is described by its energy landscape, are encoded in the

171 sity of these series-tunneling junctions can be described by J(V) = J0(V) exp(-beta1d1 - beta2d2), wh

172 The cellular automata model was described by John von Neumann and his friends in the

173 , banana and strawberry) while the remainder were described by less pleasant flavours, such as chemic

174 e large-scale dynamics of the microbiome can be described by many of the tools and observations used

175 This dependence is described by Marcus theory with a reorganization ener

176 The large ensemble of particles is described by mass action laws.

177 The formation of four adducts were described by mass spectrometry, but monoDOPAC-monoM

178 ms in graphene and in topological insulators are described by massless Dirac equations.

179 he system is linear and time-independent and is described by materials with a scalar dielectric funct

180 The bonding in such complexes can be described by means of sigma-hole interactions.

181 nt in high glycine and, therefore, could not be described by mechanisms with only one fully liganded

182 underlying movements of ultrasonic calls can be described by modules.

183 electivities obtained in these reactions can be described by NBO charges, the IR carbonyl stretching

184 The theory of this method is described by Nernst-Planck-Poisson finite element sim

185 Many physical systems are described by nonlinear differential equations that a

186 pattern formation in developing embryos can be described by nonlinear reaction-diffusion equations.

187 Protein dynamics are described by normal mode analysis based on a simplif

188 at evade mean field order have, in contrast, been described by Onsager's theory of the reaction field

189 cal systems, but also to any system that can be described by ordinary differential equations.

190 astic-solid mechanics for materials that can be described by ordinary elasticity tensors.

191 and urine from Fabry patients have recently been described by our group.

192 40) large tumor antigen (Tag) has previously been described by our laboratory for scenarios of recomb

193 ld, as their backbone structure can uniquely be described by parametric equations.

194 NAFLD recurrence was described by performing a blinded reevaluation of po

195 A minimal core surface microbiota is described by persistence through development and by s

196 8% of total mercury (HgT) log Kd variability was described by porewater dissolved organic carbon conc

197 en individuals and populations cannot easily be described by predefined numbers.

198 m, but rather as geometric shapes that could be described by principles of physics and mathematics.

199 nces of animals are often structured and can be described by probabilistic transition rules between a

200 The SAXS data for pure RL micelles can be described by prolate core-shell structures with a cor

201 ted hypoxia-responsive drug-delivery vehicle is described by Q.-D. Shen, Z. Gu, and co-workers on pag

202 Less genomic variation for kyphosis was described by QTL regions and no region was associate

203 iration of the leaf and canopy, by contrast, is described by quasilinear, empirical relations for the

204 nthesis of a new amino acid phosphonium salt was described by quaternization of melting triphenylphos

205 rized by a fixed effect, and time dependency is described by random effects.

206 adaptation of visual cortical responses can be described by recurrent network connections with fixed

207 South Africa), and predicted mortality rates were described by region at 0-3, 3-6, 6-12, 12-24, and 2

208 transcription start sites, in a way that can be described by repositioning of the single-stranded tra

209 he species involved in these transformations are described by resonance structures that suggest beta-

210 monstrations that evolutionary dynamics must be described by selection at various levels in the hiera

211 iagnostic accuracy for each LI-RADS category was described by sensitivity, specificity, and positive

212 nts to solve this task, in a manner that can be described by several distinct behavioral phases.

213 Facilities were described by several attributes including provider

214 islands mysteriously moving around on lakes were described by several Latin authors almost two mille

215 biomacromolecular core-shell crystal growth is described, by showing that these crystals can be asse

216 These systems are described by simplicial complexes.

217 e course of change in fluorescence intensity were described by single exponentials.

218 Rheological properties are described by standard viscoelastic models and the pa

219 high-frequency limit of the drive, topology is described by standard topological invariants, such as

220 icle and the small magnetic particle pattern is described by stochastic moves over the surface of the

221 Less distinct topography has been described by studies that deviated from the formula

222 fast growing peritoneal metastases can only be described by such a complex partial differential equa

223 the number of parasites per host individual is described by Taylor's law (TL) or the negative binomi

224 Two key experimental quantities of PEG are described by the model: the ratio of single channel

225 The protein restraints are described by the quadratic elastic network model.

226 contractions of distinct actin architectures are described by the same master curve when considering

227 imes, and concentrations shows that the data are described by the Sand equation and that migration ef

228 The massless solutions to the Dirac equation are described by the so-called Weyl Hamiltonian.

229 sical magnetism, among the many systems that are described by the XY Hamiltonian.

230 These clear discriminations can be described by the ability of a bacterium to change its

231 gas into a quasi-equilibrium state that can be described by the Bose-Einstein statistics.

232 Quantum spin liquids cannot be described by the broken symmetries associated with co

233 tion of temperature and Ge concentration can be described by the cBOmega thermodynamic model.

234 al change at approximately 13 GPa and cannot be described by the conventional network structure of ic

235 vel form of band crossing, the new TM cannot be described by the established results that characteriz

236 ge steady-state limiting current is shown to be described by the familiar expression for a generator-

237 fundamental relationships and that they can be described by the homologous series nFeO.mFe2O3.

238 results show that the pattern formation can be described by the identification of domains that can b

239 tate flows through multiple channels and can be described by the kinetic partitioning mechanism.

240 attern of connectivity among populations can be described by the measurement of a dispersal kernel.

241 y discovered classes of relaxors that cannot be described by the polar nanoregion model, and provides

242 not well-separated excess charges and cannot be described by the prevailing classical picture.

243 s decreased with increase in pH, which could be described by the speciation of Fe(VI) and Trp (or Kyn

244 ordinate used to monitor the transition, can be described by the splitting probability, p(fold)(x).

245 x mode of snake locomotion, sidewinding, can be described by the superposition of two waves: horizont

246 dependence between 67 and 106 bp that cannot be described by the worm-like chain model.

247 oteins, such allosteric regulation has often been described by the concerted Monod-Wyman-Changeux and

248 MM potentials, where the chemical system has been described by the M06-2X functional and the environm

249 (CSF) cavity within the conus medullaris has been described by the term ventriculus terminalis (VT) o

250 n optical fibers whose propagation evolution is described by the 3NLSE.

251 serve a liquid-like magnetic response, which is described by the coexistence of two disordered magnet

252 y leads to significant spin splitting, which is described by the Dresselhaus term, at both the conduc

253 A new concept in anionic 10 pi aromaticity is described by the embedding of a compensating charge w

254 os and - [Formula: see text] of purified mCP is described by the following functions: e 1 = -0.004363

255 This is described by the force-frequency response (FFR), a ch

256 m and collective phenomena if their dynamics is described by the general super-Arrhenius relation.

257 be engineered so that its intrinsic physics is described by the generalized Ising model and can enco

258 in the intracellular and interstitial spaces is described by the intermediate component, whereas the

259 illations in noisy spatial population models is described by the Ising universality class of statisti

260 ffective refractive index and the modal gain is described by the linewidth broadening factor, which i

261 electrons at the metal-insulator transition is described by the Mott criterion.

262 ameters of the parent protonated ligands; it is described by the mutual contribution of the NBO charg

263 uction in a fundamentally different way than is described by the PGM.

264 nux computers and find that in both cases it is described by the same scale-free power-law distributi

265 The photochemistry is described by the superposition of two independent par

266 Gene activity is described by the time series of discrete, stochastic

267 erm data of Cr(VI) adsorption on WB and M-WB was described by the Freundlich adsorption model.

268 Body kinematics was described by the leg and trunk segment angles in the

269 99.0% of the variation between the spectra were described by the first two principal components (PC

270 , and temperature T of solid-state materials are described by their equations of state (EOSs), which

271 s, and their contributions to knowledge, can be described by their depth (specialized, domain-specifi

272 ransformations in other systems can likewise be described by these models, and thus our findings sugg

273 ampullate silk fibers, under any conditions, are described by this single parameter that connects the

274 Here, we show that this reaction can be described by three coefficients: association of capsi

275 that TcpP diffusion is heterogeneous and can be described by three populations of TcpP motion: one fa

276 increase in the chloride current (ICl ) that is described by titration of a protonatable site with pK

277 ll features associated with the fractal gaps are described by two integer topological quantum numbers

278 s found that this multisensory transform can be described by two basic principles: unisensory informa

279 ts from an Ir oxo/oxyl intermediate that may be described by two competing bonding models, which are

280 The reversible glyoxal uptake can be described by two distinct reservoirs for monomers and

281 been probed by theoretical calculations, can be described by two horizontally sigma-bonded 2p(x) and

282 d systemic glucose during the episodes could be described by two significantly distinct parallel line

283 demonstrate that the dynamics of the ligand is described by two relaxation times, one of which arise

284 in the highly destabilizing lesions Gh or Sp is described by two sequential first-order reactions, in

285 r the synthesis of 2-aryl-3-sulfonylchromans is described by two-step routes: (i) NH4OAc mediated Kno

286 Ordinal values of BE and breast density were described by two independent readers by using the B

287 materials, which host quasi-particles which are described by ultrarelativistic Dirac-like equations,

288 s (ddBCNAs) with d-chirality have previously been described by us to inhibit replication of human cyt

289 nd -OH) to the corresponding nitro compounds is described by use of nonanebis(peroxoic acid).

290 The donor cell state transitions can be described by using a stochastic model, which predicts

291 ally, we discuss how TP53 alterations should be described by using accurate nomenclature to avoid con

292 etailed calculation of mean cumulative count is described by using a simple hypothetical example, and

293 roughout the geographic range of the species was described by using sequence data from 13 loci.

294 The dissipation rates of kresoxim methyl were described by using first-order kinetics and its hal

295 polar peroxide formation could largely (70%) be described by variation in fatty acid composition and

296 properties of layered nanocomposites cannot be described by volume fraction considerations alone and

297 Physical water scarcities can be described by water stress indices.

298 ough samples with random inhomogeneities can be described by way of transmission eigenchannels, which

299 A detection scheme is described by which the histamine contents of biologic

300 ze strong-force dynamics in Bloch bands that are described by Wilson lines and observe an evolution i