戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (1語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1  analysis suggested that program culture may be described by 2 components: Wellness and Negative Expo
2             Combinatorial chromatin patterns were described by 42 major chromatin states with selecte
3                          The four VS domains are described by a continuum electrostatic model under v
4        The electronic properties of graphene are described by a Dirac Hamiltonian with a four-fold sy
5                        The sequencing counts are described by a lognormal-beta-binomial hierarchical
6                   The effects of irradiation are described by a modified version of the linear-quadra
7                             Our measurements are described by a new model where the Poisson ratio dri
8                            Reaction kinetics are described by a rapid, low-fractionating uptake step
9           Bivalve, ammonite and snail shells are described by a small number of geometrical parameter
10 h as the Type Iax-class prototype SN 2002cx, are described by a variety of models such as the failed
11                    We find that peptoids can be described by a "rotamer" treatment, similar to that e
12 ical, and the molecular spacing for both can be described by A = 1.42 +/- 0.02 nm, B = 1.32 +/- 0.02
13 luctuating stimuli is largely linear and can be described by a biphasic temporal filter and dynamical
14          At pressure <6 GPa, the PAW-GGA can be described by a Birch-Murnaghan equation of state with
15 t boundary diffusion in helical peptides can be described by a classical, Einstein-type, 1D diffusion
16 ial antimicrobial susceptibility may need to be described by a combination of parameters rather than
17 ned by a single cooperative pathway, but can be described by a competitive two-pathway mechanism.
18 that crystalline doxorubicin dissolution can be described by a first order rate constant of 1.0x10(-9
19  across different vegetation communities can be described by a Fourier model.
20 ic behavior of the solid-phase reactor could be described by a fractal Michaelis-Menten model with a
21  firmly established that protein folding can be described by a funneled energy landscape.
22  of structural formation was studied and can be described by a generalized model of nucleated polymer
23             This quantitative dependence can be described by a Hill equation, with a Hill coefficient
24                    While the system can only be described by a large hierarchical set of equations in
25 easured for MBD3 bound to methylated DNA can be described by a linear combination of those for the me
26   Antibody responses in African children can be described by a model 15 including both short-lived AS
27 t all the studied sites and could adequately be described by a modified form of the angstromngstrom t
28                 Globally, the datasets could be described by a monomer-dimer-tetramer-hexamer or a mo
29           Complex economic systems can often be described by a network, with nodes representing econo
30  pH 8 at both oxic and anoxic conditions can be described by a new model that incorporates Fe(II) rel
31  the intrinsically nonequilibrium system may be described by a non-Hermitian Hamiltonian.
32 hat (1) the crystal structure of PFWO should be described by a partly ordered cubic perovskite (i.e.
33 n a population and its environmental cue can be described by a population-level reaction norm.
34 dence suggests that cytoplasmic rheology can be described by a poroelastic model, in which the cytopl
35  of ORN activation, the fly's locomotion can be described by a random walk model where a fly's moveme
36                              This effect can be described by a recently proposed magnonic mechanism(1
37  with HNO3/nitrate surface density and could be described by a simple analytical equation.
38 aditional drugs, where target engagement can be described by a simple bimolecular equilibrium equatio
39                            The reactions can be described by a simple mechanism that merges known beh
40 s classical organellar proteomics and cannot be described by a single and ultimate list of protein co
41                     Results show signals can be described by a single linear transition path with dif
42      The sampling and extraction of WSOC can be described by a single parameter, P, expressing the ra
43 currently thought that filament kinetics can be described by a single rate constant for each end.
44 olution of gene blocks in proteobacteria can be described by a small set of events.
45  forms a three-dimensional scaffold that can be described by a space group.
46 exity of this multiscale correspondence, can be described by a sparse subset (approximately 200) of g
47 hanistic complexity of the linker region can be described by a spring model with Brownian motion of t
48 susceptible-infected-recovered mechanism can be described by a stochastic birth-death process of Galt
49 at photo-activated electron transport cannot be described by a superposition of the properties due to
50                          These phenomena can be described by a theoretical model in which the periodi
51 rature and organismal performance, which can be described by a thermal performance curve.
52 ows weak net directional movement, which can be described by a thermodynamic sink arising from the di
53                         These dynamics could be described by a three-state model involving stochastic
54 he presence of gene flow, a phylogeny cannot be described by a tree but is instead a directed acyclic
55  Overall, bacterial phenotypic evolution can be described by a two-stage process with a rapid initial
56            These striated 2D crystals cannot be described by a typical unit cells of 1-2 angstrom for
57 ial swarms and the spreading of biofilms can be described by a unified biophysical theory that involv
58 nding within the [W(mu-H)Si(mu-H)W] core can be described by a variety of resonance structures, some
59         The regulation of their activity has been described by a hierarchical model in which elements
60 ns responsible for the OSE have historically been described by a two-level dressed-atom model, which
61 iezoelectric fields associated with the SAWs being described by a relatively simple classical relaxat
62 ollected using cw laser excitation at 785 nm is described by a 300 K thermal distribution of excitati
63 that directional guidance along fibre tracts is described by a bimodal von Mises-Fisher distribution
64 ing that the two-dimensional electron system is described by a Bloch Hamiltonian, system is insulatin
65 tion to an easy-plane antiferromagnet, which is described by a Bose-Einstein condensation of magnons.
66 am having multiple degrees of freedom (DoFs) is described by a coherency matrix G spanning these DoFs
67                             The design space is described by a computational grid where every cell ca
68                                           It is described by a continuously varying power law exponen
69           The mobility in this linear regime is described by a creep model of zero-dimensional charge
70                               The meta-layer is described by a flexural wave polarizability tensor, w
71 e two strategies, A and B, whose interaction is described by a general payoff matrix.
72  strain-generated signaling molecule, and it is described by a kinetic multi-stage model.
73 rders of magnitude with Fe(II)/Fe(total) and is described by a linear free energy relationship.
74 tical framework in which a real-world system is described by a low-dimensional equation system with a
75  in the absence of magnetic anisotropy terms is described by a Mobius transformation in complex stere
76 istics observed in the native membranes, and is described by a multisquare model with Schiff base dep
77 tacts that are about to slide, whose density is described by a nontrivial exponent [Formula: see text
78 t z 2, typical of a Lifshitz transition, but is described by a nontrivial interacting fixed point.
79 ram-scale synthesis of 3-sulfonyl flavanones is described by a one-pot straightforward POCl(3) mediat
80 rection and magnitude of the resulting shift 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               This antitumor immune response is described by a primary and a secondary (or memory) re
83        Each entity (agent, lectin or ligand) is described by a range of properties that are summarize
84 on of stepping durations of KIF3AC molecules is described by a rate (k (1) = 11 s(-1)) without appare
85 EVOO's) endogenous polyphenols; the reaction is described by a sigmoidal curve.
86                                   The factor is described by a simple linear combination of buried su
87  second-harmonic generation intensity, which is described by a simple model that accounts for the int
88 or the synthesis of pyrrolo[1,2- a]azaarenes is described by a straightforward HOAc-mediated double c
89 species to show that avian trophic diversity is described by a trait space with four dimensions.
90 tercalators, we find that ligand association is described by a two-step process, which consists of fa
91 a positive threshold Q in the inertial range is described by a universal q- exponential function, P(t
92 , the control of ion flow by the gate domain is described by a vapor-lock mechanism, and the simple c
93                Between treatment variability was described by a mixed effects model.
94 lted in kinetic isotope fractionation, which was described by a Rayleigh model with an enrichment fac
95 The loss of vitamin D(3) during storage time was described by a second order reaction.
96                     The system heterogeneity was described by a three-dimensional ( x, y, z) surface
97                        Maternal dolutegravir was described by a two-compartment model linked to a fet
98 a ganglion cell's excitatory synaptic inputs were described by a divisive interaction between excitat
99                                  The results were described by a kinetic model allowing the simultane
100                Rifampicin CSF concentrations were described by a partition coefficient (5.5% [95%CI 4
101                Rifampicin CSF concentrations were described by a partition coefficient (5.5%; 95% con
102 e mobile segment of troponin-I to troponin-C were described by a simple kinetic scheme.
103  The surface pressure decay during depletion were described by a stretched exponential that suggested
104 showed that the displacements of these seals were described by a truncated power law distribution acr
105     The X-ray spectrum is ultra-soft and can be described by accretion disk emission with luminosity
106                    The burden of illness can be described by addressing both incidence and illness se
107 gical management for acute anxiety and pain, are described by age and development.
108 butions of histopathology and polyp location were described by age and gender.
109                       Chemical reactions can be described by an energy diagram along a reaction coord
110 chromosome structures are fluid and can only be described by an ensemble, which is consistent with th
111                  Other experiments could not be described by an equilibrium model, suggesting that a
112 llow a similar spatial dependence, which can be described by an HA-dependent potential gradient; PIP2
113 e across all animals and time points and can be described by an inverse power law.
114 nic ground state of the Au25(SC8H9)18(-) MPC is described by an eight-electron P-like superatom orbit
115 quilibria between VOC and water vapor, which is described by an extended Manes method.
116  and the equilibrated repressor-bound states is described by an extension of the Peccoud-Ycart two-st
117 n the two so that changes in the outcome can be described by and predicted by changes in the inputs.
118 nt numbers of human transcripts have not yet been described by annotation projects, while existing tr
119 nd anomalous supercurrent enhancement cannot be described by any known conventional phenomenon of Jos
120 istic states, massless Kane fermions, cannot be described by any other relativistic particles.
121 l order; it means that temporal order cannot be described by any pre-defined local variables.
122                 We show that the cornea must be described by at least two shear moduli, contrary to c
123     At large distances the heat transfer can be described by black body radiation, at shorter distanc
124                              The excitations are described by Boltzmann distributions with their fact
125                          Infant dolutegravir was described by breastmilk-to-infant and infant elimina
126 ess cost C and the resistance ratio Rr could be described by C = 24.47/(1 + exp([1.57 - Log10Rr]/0.2)
127 under supersaturated water vapour conditions is described by classic Kohler theory.
128 eproducible electrochemical signals that can be described by classical electrochemical theory as well
129 etre dimensions exhibit features that cannot be described by classical electrodynamics.
130 hat the nucleation of amyloid fibrils cannot be described by classical nucleation theory: in the two-
131 nmental (plant leaves and sand) surfaces can be described by classical sorption isotherms.
132                      Phage-sand interactions were described by colloidal filtration theory and the ex
133                 Niche differences could only be described by combinations of traits, corresponding to
134 ults demonstrate that brain adaptability can be described by common processes that drive the dynamic
135 in the field of photocatalytic carbonylation is described by compiling the literature of the last 40
136 or interquartile range, and precision should be described by confidence intervals; S.E. should not be
137                         The observed results were described by considering the potentials of redox pa
138 targets and functions of ubiquitylation have been described; by contrast, few targets of NEDD8 have b
139 nanodots toward the electroreduction of H2O2 was described by cyclic voltammetric and amperometric te
140                                          KCl is described by Debye-Huckel screening and a Manning con
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 lutes in nonreactive porous media can mostly be described by diffusion driven by the concentration gr
144 all of our data together, the effects cannot be described by doping alone.
145 exyl isonicotinate binding to P450 2E1 could be described by either a conformational-selection or an
146 e, bottom-up control of phytoplankton cannot be described by either one alone, nor by a combined metr
147 ic region of the dispersion the solitons can be described by envelope functions satisfying the nonlin
148 discover self-similar properties that cannot be described by existing models and discuss possible sce
149           The transient plasticity of period was described by existing mathematical models of the Ara
150                        Atomic configurations were described by feature matrix based on internal vecto
151 al 180(o) commensurate magnetic domains, can be described by ferromagnetic and ferroelectric domains
152                      Doxorubicin leakage can be described by first order rate constant for transport
153 he behavior of individual molecular formulas was described by fitting the single exponential model to
154  average neck size, [Formula: see text], can be described by [Formula: see text], where [Formula: see
155                  The CO2 emission reductions are described by g CO2/km emission targets for average n
156 models appear in TIGRFAMs, while 628 systems are described by Genome Properties.
157 re colony geometry and public good diffusion are described by graphs.
158              Treatment effects on PFS and OS were described by hazard ratios (HRs), median times to e
159     We report several features that have not been described by in vitro analysis of the process, chie
160                      Amorphous materials are being described by increasingly powerful computer simula
161  consists of, the functional status of which is described by 'intestinal permeability'.
162 erobserver and intraobserver reproducibility were described by intraclass correlation coefficients (I
163 erature dependence of the critical field can be described by introducing an interaction term into the
164 ider locomotion along a surface where forces are described by isotropic Coulomb friction.
165 observation times the dynamics can sometimes be described by isotropic random walks, usually the dire
166 the material's plastic properties, which can be described by its stress-strain behaviour.
167 getics of a protein's folding process, which is described by its energy landscape, are encoded in the
168 y a random walk model where a fly's movement is described by its speed and turn-rate (or kinematics).
169 sity of these series-tunneling junctions can be described by J(V) = J0(V) exp(-beta1d1 - beta2d2), wh
170 , banana and strawberry) while the remainder were described by less pleasant flavours, such as chemic
171                              This dependence is described by Marcus theory with a reorganization ener
172              The large ensemble of particles is described by mass action laws.
173                The formation of four adducts were described by mass spectrometry, but monoDOPAC-monoM
174            The bonding in such complexes can be described by means of sigma-hole interactions.
175 derivatives, under mild reaction conditions, is described by means of the use of an environmentally b
176 underlying movements of ultrasonic calls can be described by modules.
177 While regulation of AR signaling by PTEN has been described by multiple groups, it is not known wheth
178 electivities obtained in these reactions can be described by NBO charges, the IR carbonyl stretching
179                    The theory of this method is described by Nernst-Planck-Poisson finite element sim
180                        Many physical systems are described by nonlinear differential equations that a
181 at evade mean field order have, in contrast, been described by Onsager's theory of the reaction field
182 cal systems, but also to any system that can be described by ordinary differential equations.
183 astic-solid mechanics for materials that can be described by ordinary elasticity tensors.
184 ld, as their backbone structure can uniquely be described by parametric equations.
185            A minimal core surface microbiota is described by persistence through development and by s
186 n debate whether thermal transport can still be described by phonons at the Ioffe-Regel limit.
187 8% of total mercury (HgT) log Kd variability was described by porewater dissolved organic carbon conc
188 m, but rather as geometric shapes that could be described by principles of physics and mathematics.
189 nces of animals are often structured and can be described by probabilistic transition rules between a
190       The SAXS data for pure RL micelles can be described by prolate core-shell structures with a cor
191 ted hypoxia-responsive drug-delivery vehicle is described by Q.-D. Shen, Z. Gu, and co-workers on pag
192          Less genomic variation for kyphosis was described by QTL regions and no region was associate
193              The OCR determined over 21 days was described by quadratic equations, with coefficients
194 iration of the leaf and canopy, by contrast, is described by quasilinear, empirical relations for the
195 rized by a fixed effect, and time dependency is described by random effects.
196  adaptation of visual cortical responses can be described by recurrent network connections with fixed
197 South Africa), and predicted mortality rates were described by region at 0-3, 3-6, 6-12, 12-24, and 2
198 transcription start sites, in a way that can be described by repositioning of the single-stranded tra
199 he species involved in these transformations are described by resonance structures that suggest beta-
200                           Variability should be described by S.D. or interquartile range, and precisi
201 f reconnection of long straight vortices can be described by self-similar solutions of the local indu
202 iagnostic accuracy for each LI-RADS category was described by sensitivity, specificity, and positive
203 nts to solve this task, in a manner that can be described by several distinct behavioral phases.
204  islands mysteriously moving around on lakes were described by several Latin authors almost two mille
205 nce of anogenital warts (AGW) from 2010-2016 were described by sex and by the sex of sex partners.
206                      Often genetic variation is described by showing relationships among populations
207  biomacromolecular core-shell crystal growth is described, by showing that these crystals can be asse
208 ical transitions between Landau levels (LLs) are described by simple selection rules associated with
209 rogeneous ensemble of structures that cannot be described by simple polymer theory.
210                                These systems are described by simplicial complexes.
211 es of ET over 1-2 nm in proteins can largely be described by simplified nonadiabatic theory, it is no
212 e course of change in fluorescence intensity were described by single exponentials.
213 es of most substituted fulvenes (159 of 225) are described by singly excited HOMO -> LUMO configurati
214 ation pathways of ZrT(d) and Zr(25) in water were described by small-angle X-ray scattering (SAXS), p
215                       Rheological properties are described by standard viscoelastic models and the pa
216  high-frequency limit of the drive, topology is described by standard topological invariants, such as
217 icle and the small magnetic particle pattern is described by stochastic moves over the surface of the
218  fast growing peritoneal metastases can only be described by such a complex partial differential equa
219 of experimental data for different rocks can be described by such thermally-activated mechanisms, com
220  the number of parasites per host individual is described by Taylor's law (TL) or the negative binomi
221 d gluons (the constituents of nucleons) that are described by the equations of quantum chromodynamics
222 contractions of distinct actin architectures are described by the same master curve when considering
223 The massless solutions to the Dirac equation are described by the so-called Weyl Hamiltonian.
224  of synapses and their location in the brain are described by the synaptome.
225  a wealth of quantum many-body problems that are described by the two-dimensional extended Hubbard mo
226 sical magnetism, among the many systems that are described by the XY Hamiltonian.
227              These clear discriminations can be described by the ability of a bacterium to change its
228 nal superconductors with properties that can be described by the Bardeen-Cooper-Schrieffer and the Mi
229 ends in sorption coefficients that could not be described by the basic electrostatic potential theory
230  gas into a quasi-equilibrium state that can be described by the Bose-Einstein statistics.
231 tion of temperature and Ge concentration can be described by the cBOmega thermodynamic model.
232 al change at approximately 13 GPa and cannot be described by the conventional network structure of ic
233 vel form of band crossing, the new TM cannot be described by the established results that characteriz
234 ge steady-state limiting current is shown to be described by the familiar expression for a generator-
235  fundamental relationships and that they can be described by the homologous series nFeO.mFe2O3.
236  results show that the pattern formation can be described by the identification of domains that can b
237 attern of connectivity among populations can be described by the measurement of a dispersal kernel.
238 y discovered classes of relaxors that cannot be described by the polar nanoregion model, and provides
239 not well-separated excess charges and cannot be described by the prevailing classical picture.
240 ic and orthosteric activation mechanisms can be described by the same scheme that includes transition
241 s decreased with increase in pH, which could be described by the speciation of Fe(VI) and Trp (or Kyn
242 ordinate used to monitor the transition, can be described by the splitting probability, p(fold)(x).
243 x mode of snake locomotion, sidewinding, can be described by the superposition of two waves: horizont
244 adsorption of Sb(III) on Fe(3)O(4)/HCO could be described by the synergistic adsorption of Sb (III) o
245 pper extremity recovery after stroke and has been described by the 70% proportional recovery rule for
246 o prepare iron-depleted CAMHB (ID-CAMHB) has been described by the Clinical and Laboratory Standards
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 ies to a range of bosonic systems because it is described by the focusing nonlinear Schrodinger equat
255 os and - [Formula: see text] of purified mCP is described by the following functions: e 1 = -0.004363
256                                         This is described by the force-frequency response (FFR), a ch
257 m and collective phenomena if their dynamics is described by the general super-Arrhenius relation.
258 ems in equilibrium, whose critical behaviour is described by the general theory of phase transitions.
259  be engineered so that its intrinsic physics is described by the generalized Ising model and can enco
260  use of limited neurocomputational resources is described by the inclusion of the "neurocomputational
261 in the intracellular and interstitial spaces is described by the intermediate component, whereas the
262 illations in noisy spatial population models is described by the Ising universality class of statisti
263 ffective refractive index and the modal gain is described by the linewidth broadening factor, which i
264  electrons at the metal-insulator transition is described by the Mott criterion.
265 ameters of the parent protonated ligands; it is described by the mutual contribution of the NBO charg
266 uction in a fundamentally different way than is described by the PGM.
267                           The photochemistry is described by the superposition of two independent par
268 erm data of Cr(VI) adsorption on WB and M-WB was described by the Freundlich adsorption model.
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 actions, which are ubiquitous in physiology, are described by theoretical models of receptor pharmaco
273 ransformations in other systems can likewise be described by these models, and thus our findings sugg
274 ampullate silk fibers, under any conditions, are described by this single parameter that connects the
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           In contrast, biofilm colony growth is described by transient solutions associated with a nu
278  problems in strong-correlation physics that are described by triangular-lattice Hubbard models.
279 ll features associated with the fractal gaps are described by two integer topological quantum numbers
280 s found that this multisensory transform can be described by two basic principles: unisensory informa
281 ts from an Ir oxo/oxyl intermediate that may be described by two competing bonding models, which are
282 been probed by theoretical calculations, can be described by two horizontally sigma-bonded 2p(x) and
283                    Loss of protein structure is described by two reaction coordinates: conformational
284 r the synthesis of 2-aryl-3-sulfonylchromans is described by two-step routes: (i) NH4OAc mediated Kno
285 antioxidant effects of OAE and of a pure BZF were described by two perfectly overlapping curves whose
286  materials, which host quasi-particles which are described by ultrarelativistic Dirac-like equations,
287 s (ddBCNAs) with d-chirality have previously been described by us to inhibit replication of human cyt
288 nd -OH) to the corresponding nitro compounds is described by use of nonanebis(peroxoic acid).
289         The donor cell state transitions can be described by using a stochastic model, which predicts
290 ally, we discuss how TP53 alterations should be described by using accurate nomenclature to avoid con
291 lid areas at follow-up, then the cyst should be described by using standardized terminology.
292                    The coupled phenomena can be described by using the unsteady convection-diffusion-
293 etailed calculation of mean cumulative count is described by using a simple hypothetical example, and
294 ction of interleukin 1alpha cancer biomarker was described by using epoxy-substituted polythiophene p
295                           Body weight change was described by using linear mixed models, including bi
296 polar peroxide formation could largely (70%) be described by variation in fatty acid composition and
297  properties of layered nanocomposites cannot be described by volume fraction considerations alone and
298                Physical water scarcities can be described by water stress indices.
299 ough samples with random inhomogeneities can be described by way of transmission eigenchannels, which
300 ze strong-force dynamics in Bloch bands that are described by Wilson lines and observe an evolution i

 
Page Top