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1 lization of the treatment variable (exposure coarsening).
2 vidence for the realizability of accelerated coarsening.
3 ying reduction in diffusion, which restricts coarsening.
4 o fragment into independent particles during coarsening.
5 lved in foaming, emulsification, and droplet coarsening.
6 lacements-per-atom (dpa) with moderate grain coarsening.
7 n of the AgNPs and inhibited aggregation and coarsening.
8  to 3 also promoted particle aggregation and coarsening.
9  subnetwork that may be utilized for further coarsening.
10 ium, representing a new approach to directed coarsening.
11 fail to reproduce temporally correct network coarsening.
12 s of modern theories of diffusion-controlled coarsening.
13 h, the actin cytoskeleton showed only subtle coarsening.
14 clusters lower surface tension and slow down coarsening.
15 and inert forms, can drive faster condensate coarsening.
16 te at near-melting temperatures with minimal coarsening and creep deformation.
17 al bonding with the Au NPs and inhibit their coarsening and deactivation.
18 es, dynamically arresting the progression of coarsening and deforming the membrane.
19 in situ TEM to directly observe and study NP coarsening and differentiate Ostwald ripening from coale
20  and provide a possible mechanism for domain coarsening and eventual molecular alignment in monolayer
21 c nature of the transformation including the coarsening and facet regulation process are still poorly
22                                     The twin coarsening and heterogeneous recrystallization resulted
23 can protect the crystalline particle against coarsening and oil drainage.
24 atio and roughness indicating that nanosheet coarsening and the associated changes in the external (m
25 ial processes, and their geometry, drainage, coarsening, and rupture strongly affect those operations
26 e broad implications for droplet nucleation, coarsening, and size control in chemically driven fluids
27 of individual NC structure and inhibition of coarsening are key, e.g., for avoiding catalyst degradat
28 but their utility as catalysts is limited by coarsening at high temperatures.
29 oskeletal actin networks exhibit significant coarsening, attendant with decreasing average mechanical
30  leads to differences in both morphology and coarsening behavior of the nanoparticles that we used to
31 with distinct metal-support interactions and coarsening behaviors.
32 sites for boundaries, drastically alters the coarsening behaviour of the system; particularly when co
33 ductivity has a significant influence on the coarsening behaviour of various systems of grains, due t
34 at the ability to induce rapid biocondensate coarsening can be advantageous in synthetic-biological c
35 the number of metal atoms that can engage in coarsening can be controlled with this technique, and TE
36 f these topologically complex systems during coarsening can be quantified by measuring the probabilit
37                                 This dynamic coarsening can be understood heuristically as the result
38  combining both SC- and nucleoplasm-mediated coarsening can explain crossover patterning in wild-type
39 litate droplets' nucleation but hinder their coarsening due to the coupled motion between droplets an
40 ave a large ligament size due to substantial coarsening during dealloying at high temperature.
41 ation, 3D potassium islands with further SEI coarsening during plating/stripping, possibly dead potas
42 t-order phase transition in which late-stage coarsening dynamics are mediated by Brownian coalescence
43  phenomena are always strongly implicated in coarsening dynamics but are, in detailed-balance systems
44 uantum phase transition, but rather a faster coarsening dynamics in an effective two-dimensional XY m
45 t this additional term has modest effects on coarsening dynamics, but alters the static phase diagram
46                                              Coarsening dynamics, surface tension, and coalescence ki
47 ng on the type of barite used, an additional coarsening effect or a strong formation of oriented aggr
48 e depletion interactions dominate the system coarsening; elastic interactions no longer prevail.
49                                   We present coarsening experiments on wet foams, with liquid fractio
50 the distinctive association of progressively coarsening facial features, relative macrocephaly, and t
51                            One key aspect of coarsening following a quench below the critical tempera
52 Distinct from existing models, iHerd's graph coarsening for hierarchical learning allows us to succes
53 s that embody the information contained in a coarsening grain network.
54 n, which is associated with anisotropic twin coarsening, heterogeneous recrystallization, and high st
55 dentify the mechanism behind Pt nanoparticle coarsening in an aqueous environment.
56  to the formation of grain boundaries during coarsening in nanoporous metals.
57                                      Data on coarsening in Ni-Al alloys is examined.
58 e of 1,8-diiodooctane and the rate of domain coarsening in the plasticized film which helps elucidate
59 d then progress within seconds to late stage coarsening in which domains grow via two mechanisms 1),
60                  We also discuss modeling of coarsening including diffusion and decay of individual N
61 mulators, which we leverage here to reveal a coarsening-induced breakdown of Kibble-Zurek scaling pre
62 are good model systems for investigations of coarsening-induced structures, because the continuous li
63                                              Coarsening is a ubiquitous phenomenon that underpins cou
64 olution of ordered domains, we show that the coarsening is driven by the curvature of domain boundari
65                                         This coarsening is even more pronounced when both reactants a
66                                              Coarsening is markedly curtailed, and the jammed colloid
67 ain walls, and that domain straightening and coarsening is predominantly driven by the relaxation and
68                         Here, a new model of coarsening is presented, involving diffusive transport t
69                             Thus, mechanical coarsening is suitable for the PEMFC system.
70 e we report atomic-scale observations on the coarsening kinetics of MGNs at high temperatures by in s
71                        Here we show that the coarsening kinetics of NiAl-type precipitates is in exce
72 n-oxidizing bacteria revealed an alternative coarsening mechanism in which adjacent 2- to 3-nanometer
73 ants likely acts through the same underlying coarsening mechanism, differing only in the spatial comp
74                                 However, the coarsening mechanisms of metallic glass nanoparticles (M
75 n content of both synthetic and experimental coarsening microstructures as quantified by both a compu
76 ese results are consistent with an anomalous coarsening model for island growth.
77 zyp1 mutants, which lack an SC, we develop a coarsening model in which crossover precursors globally
78 xplained by a predictive, diffusion-mediated coarsening model, in which large, approximately evenly-s
79  results of the present study reconcile with coarsening models from the Lifshitz-Slyozov-Wagner theor
80 DL performance, and observe that the feature coarsening not only decreases the training time by [Form
81   Here, we observed universal scaling in the coarsening of a homogeneous two-dimensional Bose gas, wi
82 ction dependence during diffusion-controlled coarsening of a polydisperse assembly of particles have
83 owever, the task of identifying a predictive coarsening of an ecosystem is distinct from the task of
84                                              Coarsening of an isolated far-from-equilibrium quantum s
85 rve a gradual growth of correlations through coarsening of antiferromagnetically ordered domains(6).
86 omic force microscopy (TM-AFM) can drive the coarsening of Au nanoparticle assemblies on silicon surf
87                                          The coarsening of crystalline nanoparticles, driven by reduc
88 ity and significantly suppresses the thermal coarsening of dealloyed nanostructure.
89 will strongly influence the condensation and coarsening of drops on soft polymer films, and has poten
90 daughter cracks in striking analogy with the coarsening of finger patterns observed in nonequilibrium
91 and the strong volume-fraction dependence of coarsening of gamma precipitates in an ordered gamma' ma
92                                          The coarsening of Li2 O2 nanoparticles occurs via both conve
93 g and dealloying process, which involves the coarsening of nanoparticles and consequent facet regulat
94              Grain boundary formation during coarsening of nanoporous gold (NPG) is investigated wher
95 enabled to develop raft microdomains through coarsening of nanorafts.
96 d absence of an effect of volume fraction on coarsening of ordered gamma' (Ni3Al) precipitates in a d
97                     Fyn deletion resulted in coarsening of podocyte foot processes and marked attenua
98 support the long-standing debate that if the coarsening of Ptnano from crystal migration and coalesce
99 d representation of tundra heterogeneity and coarsening of spatial scale.
100                                Thus, despite coarsening of the actin cytoskeleton and depressed ATP l
101                                          The coarsening of the amorphous nanoparticles takes place by
102                               The growth and coarsening of the eta' precipitates caused rapid depleti
103 modulated by a dynamic interplay between the coarsening of the evolving droplet phase and the interac
104 her tissues, including lymphoid hyperplasia, coarsening of the facies, and increased body fat.
105 protofibrils form large bundles that cause a coarsening of the fibrin network due to an increase in f
106 eal that crystallization occurs prior to the coarsening of the HDL and LDL domains, obscuring the dis
107 urfactant alone did not effectively suppress coarsening of the KTP-rich phase.
108 n each section decreases slightly due to the coarsening of the microstructure from the initial layer
109 moval of the surface hydration layers causes coarsening of the nanoparticles.
110 s of two stages: (I) nucleation, growth, and coarsening of the particles to yield a single particle i
111 s from 7.2% to above 8.7% as a result of the coarsening of the phase domains.
112  This limit is set by the onset of the rapid coarsening of the precipitates and consequent loss of me
113 ory field gives rise to chain formation with coarsening of these chains into long fibers.
114 active droplets and support a model in which coarsening of these droplets via protein translocation a
115                                              Coarsening of these local features is energetically cost
116                                              Coarsening of two-phase systems is crucial for the stabi
117 d possible by the rafting (i.e., directional coarsening) of gamma ' particles that facilitates disloc
118            We evaluate the impact of feature coarsening on DL performance, and observe that the featu
119                                   Mechanical coarsening on the surface of the PMMA results in improve
120                                              Coarsening or Ostwald ripening occurs in a vast array of
121 cancies between ribbons of endothelial cells coarsening over time.
122                           In the presence of coarsening, performing a sensitivity analysis over a ran
123   We propose a new comprehensive view of the coarsening phenomenon in wet foams.
124                              We propose this coarsening process explains many aspects of Arabidopsis
125                      Much is known about the coarsening process in two-phase mixtures consisting of a
126                                         This coarsening process is assisted by thermal annealing and
127 nd a phenomenon akin to Ostwald ripening - a coarsening process seen in many systems that undergo pha
128 nto a global contractile state via an active coarsening process, in contrast to the flow transition d
129  2D dislocation loops, implying a continuous coarsening process.
130  this curvature space that is induced by the coarsening process.
131 o observe intermediate structures as part of coarsening processes that lead to the formation of singl
132 cycles that form through exponentially rapid coarsening processes, depending on the parity of the cyc
133 d decay of individual NCs and unconventional coarsening processes.
134 e saturation concentration, sharply arrested coarsening, rapid mixing, high exchange rate, and resist
135  oxides are likely to slow the morphological coarsening rate by hindering the surface diffusion in th
136      Self climb significantly influences the coarsening rate of defect networks, with important impli
137                               The subsequent coarsening rate was primarily surface diffusion controll
138 l, and applicable to many systems undergoing coarsening, regardless of their topology.
139             However, bias risk from exposure coarsening remains even without adjustment.
140  precipitates that has enabled us to develop coarsening resistant high-temperature alloys that are st
141 wavelength regions, growing the structure by coarsening, resulting in a broad distribution of domain
142                                              Coarsening results in a decrease in the interfacial area
143  correlation times associated with different coarsening scenarios.
144  particular, we develop an efficient feature coarsening technique to extract the most representative
145 ng of the film shows the mechanism of domain coarsening that potentially links to phase transition of
146 s and allowing us to explain at long term by coarsening the formation of cellular structures.
147 gglutination and droplet scavenging, thereby coarsening the grain size distribution.
148 erin to map the model onto the Cahn-Hilliard coarsening theory.
149 ting odd grains, and a transition from grain coarsening to grain self-fragmentation in the dynamical
150 sliding and rotation and by inhibiting grain coarsening, under extremely long-term creep conditions.
151 used on meso-scale bigradational sequence (a coarsening upward followed by a fining-upward sequence r
152                   Phase-field simulations of coarsening using a computationally generated structure w
153 he free energy of NC ensembles is lowered by coarsening which can involve Ostwald ripening or Smoluch
154 ause bed incision is accompanied by sediment coarsening, which facilitates development of large dunes
155 1.3 mum in KCl-MgCl(2) from 1 to 16 h due to coarsening, while remaining ~ 0.4 mum in KCl-NaCl during

 
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