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1 sannotation arises, a process we term 'error percolation'.
2 artments) or to anomalous diffusion (such as percolation).
3 , and support an extended picture of network percolation.
4 obustness by extending the deduction in core percolation.
5 he network size can indeed exhibit explosive percolation.
6 s to reside in isolated pockets that prevent percolation.
7 works, and emerges because of the asymmetric percolation.
8 l set of influencers in networks via optimal percolation.
9 static threshold due to deformation-assisted percolation.
10 hould guard against deformation-driven fluid percolation.
11 re consistent with critical gelation through percolation, additional rheological and structural prope
12 ics, and rheology to describe ion and charge percolation, adsorption of ions, and redox charge storag
13 e ice core was a challenge because meltwater percolation also affects the traditionally used paramete
14                                   Electrical percolation also plays a significant role in producing t
15                 Through detailed fractal and percolation analyses of MG structures, derived from simu
16 d on the signed similarity, we carry out the percolation analysis on this signed unipartite network,
17     We relate these observations to directed percolation and argue that Re (1) marks the onset of inf
18                                Network-based percolation and chain-binomial simulations of susceptibl
19 kinetic or dynamic arrest, phase separation, percolation and jamming.
20  immediate-release because they resist fluid percolation and penetration.
21 ee different extraction methods (maceration, percolation and Soxhlet).
22 diffusion-limited aggregation, self-avoiding percolation, and cellular automata.
23  replica theory, cavity reconstruction, void percolation, and molecular dynamics, we obtain insights
24                      The synchronization and percolation are associated to abrupt transitions, and th
25 m crack clusters or larger effective cracks, percolation at finite packing is expected when the shear
26 ption pattern can indeed result from network percolation; but this can sometimes be initiated by a lo
27 r the experimental observation of electrical percolation caused by continuous jackstraw-like physical
28 ersion efficiency is achieved by introducing percolation channels of large pores in the mesoporous Ti
29 s not random but metal ions cluster, forming percolation channels through a partly broken network of
30 onstrate that metal ions nano-segregate into percolation channels, making this a universal phenomenon
31             A specific class of fractal, the percolation cluster, explains the structural details for
32  extreme fluctuations in the geometry of the percolation cluster.
33 percolation threshold and characteristics of percolation clusters formed by subsets of atoms, which c
34 d in batch assays and breakthrough curves in percolation column experiments.
35                                          The percolation concept will underpin the design of devices
36                 The sieving models predict a percolation cutoff radius of the order of 50 nm for part
37  gel network in the cell must have a minimum percolation cutoff size exceeding 17.5 A and does not im
38 inal (1989) model of dopant-assisted quantum percolation (DAQP), as developed further in some two doz
39 s have recently called for an examination of percolation, diffusion or synchronization phenomena in m
40 rigorous lava-snow interaction via meltwater percolation down into the incandescent lava causing prod
41 ombination of size, charge distribution, and percolation effects.
42 g dry matter was extracted with solid-liquid percolation equipment using non-toxic and eco-friendly e
43  previously been shown to be associated with percolation errors.
44 e percolation threshold of the lattice (in a percolation experiment, each site of an initially empty
45                                              Percolation experiments are carried out for 103 single-c
46 t, this channel network behaved as a lateral percolation filter composed of an array of cubelike stru
47                                These lateral percolation filters were shown to be efficacious in filt
48 e to the mantle, with subsequent upward melt percolation from the asthenosphere.
49                                              Percolation has always been regarded as a substrate-depe
50                                      Optimal percolation has received considerable attention in the c
51                            Although invasion percolation identifies the important impact of macro-por
52 hows a functional form indicative of spatial percolation, implying that the connectivity of TDM plays
53 sights into the onset of plasticity and void percolation in cytoskeleton.
54 rganized ways to control synchronization and percolation in natural and social systems.
55 nd develop a stochastic algorithm based upon percolation in random graphs to compute them.
56         Here we map the problem onto optimal percolation in random networks to identify the minimal s
57 llent model material for square-lattice site percolation in the extreme quantum limit of spin one-hal
58 se behavior as well as lateral diffusion and percolation in the region of coexisting gel and fluid ph
59  provided us an analytical framework of core percolation in uncorrelated random networks with arbitra
60 sa.gov/Groups/SciTech/nano/msamanta/projects/percolation/ index.php
61                                         Core percolation is a fundamental structural transition in co
62 ted for the plasma membrane, suggesting that percolation is not the factor controlling lateral diffus
63 lthough segregation of core material by melt percolation is probably not feasible in the upper mantle
64                        The pattern of stress percolation is related to the degree of heterogeneity in
65                                      Optimal percolation is the problem of finding the minimal set of
66                                   "Explosive percolation" is said to occur in an evolving network whe
67 60 degrees required for completely efficient percolation, is considerably less than the angles observ
68 e case for network liquids near the rigidity percolation, known to affect elasticity.
69 which competing organisms are represented by percolation lattice models.
70                       At about 5 mol % gA, a percolation-like transition occurred at which the line t
71                                 Close to the percolation limit this deformation is plastic similar to
72     At doping concentrations approaching the percolation limit, charge-transfer ferromagnetism can sw
73 ems: the leaching-out of the conductor and a percolation-limited membrane conductivity that results i
74                                        These percolation lithography techniques produced permanent ph
75 he idea that mitochondria are organized as a percolation matrix, with reactive oxygen species as a ke
76 sible in the upper mantle, core formation by percolation may be possible in the lower mantle.
77 trical changes were modelled, showing that a percolation mechanism could also explain atrial reentrie
78 static field-assisted carrier separation and percolation mechanism enables an unprecedented photocond
79     Overall, our results suggest a diffusive percolation mechanism for the initial events of HIV-1 en
80  in-house algorithm and a tailor-made Clique Percolation Method to extract linear and nonlinear KEGG
81 d with soymeal obtained by conventional cold percolation method utilising hexane as the extraction so
82 We then test two fluid-flow models: invasion percolation model and effective medium model.
83                   We furthermore find that a percolation model for the defects explains the defect si
84                                      The S-I percolation model is further generalized to allow for mu
85          Finally, we introduce a data-driven percolation model mimicking rumor spreading and we show
86                         Second, we compare a percolation model of internetwork cascading to three mod
87                                            A percolation model predicts that the threshold is highly
88 ies to the influence maximization problem in percolation model, it is still important to examine its
89 n of gold nanocrystals and is explained by a percolation model.
90  decreases vulnerability, in contrast to the percolation model.
91                                 This "double percolation" model has previously explained many feature
92 critical exponents between the bond and site percolation models in networks with null percolation thr
93 antitative magnetization data are fit to new percolation models, based upon random distributions of c
94 but they are identical for the bond and site percolation models.
95 hen there is increased dimensionality of the percolation network and stronger orbital overlap.
96     In an Appendix, we show that an epidemic percolation network can be defined for any time-homogene
97 with bulk-produced carbon nanofibres (charge percolation network for electron transport, and for impa
98 ductor comprising a layer of silver nanowire percolation network inlaid in the surface layer of a Die
99 sical polymer theory, with insights from the percolation network model, we illustrate the direct prop
100 diffusion is triggered by the formation of a percolation network of antisites.
101 series of simulations, we show that epidemic percolation networks accurately predict the mean outbrea
102 his paper, we outline the theory of epidemic percolation networks and their use in the analysis of st
103               Finally, we show that epidemic percolation networks can be used to re-derive classical
104                                 The epidemic percolation networks for these models are purely directe
105  to make porous nanocomposites with metallic percolation networks that have an electrical conductivit
106  corresponding probability space of epidemic percolation networks.
107 rbon distributions in rock salt require that percolation occurred at porosities considerably below th
108 he critical (minimal) value, p(c), for which percolation occurs, i.e. a cluster connecting the opposi
109 cular concerns for data correctness; if this percolation occurs, incorrect data in one database may e
110 rate that this unexpected behavior is due to percolation of a certain type of active diffusion channe
111 l marginal stabilities favor both electronic percolation of a dopant network and rigidity percolation
112 easure of real-time activity-stimulus-evoked percolation of activity through the dentate gyrus relati
113 nt transport in polymers may result from the percolation of charge carriers from conducting ordered r
114 thus require a mechanism to prevent downward percolation of dense melt within the layer.
115 al models should describe the outcome of the percolation of genetic lineages through the population p
116 ient microhabitat experiencing constant slow percolation of highly alkaline phosphate-enriched spring
117                             Evidence for the percolation of metallic melt is provided by X-ray microt
118                    Alternative models invoke percolation of molten metal along an interconnected netw
119                                              Percolation of oxygenated water prevented the proliferat
120 pressure pumping, carbonate dissolution, and percolation of soil water through the vadose zone.
121                                              Percolation of solid domains slowed down monolayer colla
122                                              Percolation of such phase coexistence in the vicinity of
123 percolation of a dopant network and rigidity percolation of the deformed lattice network.
124  prairie dog hosts and therefore, permitting percolation of the disease throughout the primary host p
125             Separation was achieved by rapid percolation of the reaction mixture over a column of mic
126               The viscosity is driven by the percolation of the solid phase domains, which depends on
127 bile shell during condensation with the slow percolation of water during evaporation through a more h
128                                              Percolation on a one-dimensional lattice and fractals, s
129 dentifies the important impact of macro-pore percolation on permeability, it does not describe the de
130 ctly solve the properties of this asymmetric percolation on random sexual contact networks and show t
131               We conclude that the theory of percolation on semi-directed networks provides a very ge
132 stic set of transition probabilities using a percolation paradigm for a susceptible-infected (S-I) ep
133 Transition, where a sample-spanning metallic percolation path is formed as the fraction of the hoppin
134 ducing an "archipelago effect" and a complex percolation path.
135                The sensitivity of conducting percolation paths to tilt-induced texture improvement is
136 icted to rely on morphological alteration of percolation paths.
137 d pi-stacks, thus leading to two-dimensional percolation pathways along the source-drain direction.
138 s present in the higher EW membranes provide percolation pathways for charge migration between DBs, w
139 etwork density that establishes the required percolation pathways for the charge carriers.
140 s not aggregate enough to create appropriate percolation pathways that prevent fast nongeminate recom
141 n rubrene is described to occur via multiple percolation pathways, where conduction is dominated by t
142 tify virus entry occurring through diffusive percolation, penetrating areas where cell junctions are
143                                 Accordingly, percolation phase transition is proposed as a new test b
144 tional connectedness, which corresponds to a percolation phase transition.
145 should be responsible for the missing of the percolation phase transition.
146 fferent reanalysis datasets, we verified the percolation phase transition.
147 r networks whose structure exhibits rigidity percolation phase transitions.
148 xperiments and the temperatures at which the percolation probability of the gel clusters is 0.36.
149 finding approximate solutions of the optimal percolation problem from single-layer to multiplex netwo
150 at approximating the solution of the optimal percolation problem on a multiplex network with solution
151 tion threshold is obtained by solving a bond percolation problem on the Voronoi diagram of the obstac
152 f the cluster sizes, different stages of the percolation process can be discerned, and these indicate
153 V transmission behaves akin to an asymmetric percolation process on the network of sexual contacts.
154 the metabolic networks can be described as a percolation process.
155 ons activated by local binding in terms of a percolation process.
156 lkali compositions, metal ion clustering and percolation radically affect melt mobility, central to u
157  in a dynamic (non-hydrostatic) environment, percolation remains a viable mechanism for the segregati
158 errida curves on random Boolean networks and percolation simulations on square lattices, we demonstra
159 stems obstructed by nanopillars; a continuum percolation system in which a prescribed fraction of ran
160 estigate two regimes, statical and dynamical percolation, that correspond to different time scales fo
161 is suggests that it is phase separation, not percolation, that corresponds to gelation in models for
162                                In electrical percolation, the passage of current through the conducti
163  for Earth's lake area-distribution based on percolation theory and evaluate these expectations with
164 ace, opening new possibilities for deploying percolation theory and stochastic subgridscale modeling
165 e, allows estimation of the crystallinity by percolation theory and the location of regions with defe
166  in the present work illustrates clearly the percolation theory applied to MGs, for example, the perc
167                                              Percolation theory can be used to understand this critic
168                We first show that a modified percolation theory can define a set of hierarchically or
169 gels formed at 32 degrees C, indicating that percolation theory does not fully capture the dynamics o
170                                   A modified percolation theory incorporating the self-assembly behav
171      Recent progress in the understanding of percolation theory points to cation-disordered lithium-e
172             Calculated spin interactions and percolation theory predict transition temperatures large
173                   A novel model derived from percolation theory suggests that phase polyphenism may h
174                   It can be deduced from the percolation theory that the compressive ductility, ec, c
175                     Here we use methods from percolation theory to develop a mathematical framework f
176                               Here, we apply percolation theory to explain the mechanism of intermito
177                                     We apply percolation theory to explain the operation of multiple-
178                       In this work, we apply percolation theory to the UK's road network using the re
179                           Using methods from percolation theory we consider both leaky immunity, wher
180                          Using a model from "percolation theory", we show that it would be highly det
181                                        Using percolation theory, the theory of competitive exclusion
182 bonaceous materials was proven to follow the percolation theory.
183      We analyzed this transition in terms of percolation theory.
184 ing independent of frequency as predicted by percolation theory.
185 vity and is consistent with predictions from percolation theory.
186 tion theory applied to MGs, for example, the percolation threshold and characteristics of percolation
187                                The ultra-low percolation threshold and self-limited fusing ability ma
188 ases as the film thickness is reduced to the percolation threshold and that the SWNT-PABS film thickn
189 opolymer nanocomposites (CPCs) with ultralow percolation threshold are designed by reducing in situ g
190 " model predicts a power-law approach to the percolation threshold at a critical packing factor of p(
191                                            A percolation threshold at which diffusion of fluid-phase
192 g the rod concentration beyond the effective percolation threshold drives the system to self-assemble
193  to dominate the signal, exactly matches the percolation threshold for hard spheres and quantifies th
194 cting SWNTs, at high density (well above the percolation threshold for metallic SWNTs) and with appro
195  a critical area fraction, which matches the percolation threshold for the immobile point obstacles.
196 h offers a simple, direct way to measure the percolation threshold for this system, which has not pre
197                               We confirm the percolation threshold in static experiments on synthetic
198                                          The percolation threshold is expressed as the diameter of th
199                                          The percolation threshold is found to be 22% GM(1) and the c
200 For obstructed diffusion the approach to the percolation threshold is marked by a large increase in n
201 hods, the obstacles are immobilized, and the percolation threshold is obtained by solving a bond perc
202 -1)) for low particle loadings, but once the percolation threshold is reached (volume percentage of 7
203 whose size rapidly grows with time until the percolation threshold is reached and the structure colla
204 ely unbundled nanotubes, near the electronic percolation threshold is required for the effective conv
205 6 sphingomyelin mix nearly ideally, with the percolation threshold locus lying close to the liquidus
206 phosphatidylcholine mix nonideally, with the percolation threshold locus lying close to the solidus.
207                                          The percolation threshold mole fraction of gel or fluid lipi
208 ably, reproduce the exact analytical optimal percolation threshold obtained in Random Struct. Alg. 21
209 micro dendrites with an ultra-low electrical percolation threshold of 0.97 vol% (8 wt%).
210  nanocomposites show a record-low electrical percolation threshold of 3.3 x 10(-2) vol%, which arises
211 ne composite formed by this route exhibits a percolation threshold of approximately 0.1 volume per ce
212 n fell below 27 degrees C, consistent with a percolation threshold of coexisting gel and liquid-cryst
213 photobleaching threshold is 0.34 and, at the percolation threshold of gel clusters, it is 0.24.
214 f approximately p(c), where p(c) is the site percolation threshold of the lattice (in a percolation e
215 owing that, at slightly above the electrical percolation threshold of the network, binding of a speci
216  22% GM(1) and the confining diameter at the percolation threshold only approximately 50 nm.
217 tions in the recovery curves at and near the percolation threshold result from extreme fluctuations i
218 py data, the simulations show that below the percolation threshold temperature of gel clusters many n
219      At a given mole fraction, the number of percolation threshold temperatures can be 0, 1, 2, or 3.
220                            By plotting these percolation threshold temperatures on the temperature/mo
221 usters, threshold temperatures-the so-called percolation threshold temperatures-are determined where
222 more like randomly packed spheres near their percolation threshold than like jigsaw puzzles.
223 gen network in articular cartilage is near a percolation threshold that gives rise to these large mec
224  second solid can be varied above or below a percolation threshold to tune the transport properties o
225  only for concentrations of mineral above a "percolation threshold" corresponding to formation of a m
226 correlation between fitnesses can reduce the percolation threshold, and correlations at the point of
227 neered networks decrease bundling, lower the percolation threshold, and enable a strong enhancement i
228 ntersecting relation and passing through the percolation threshold, can be expected to be a good appr
229                              Images reveal a percolation threshold, i.e., the point where rafts becom
230                                       At the percolation threshold, the point at which the fluid phas
231 meter describing obstructed diffusion is the percolation threshold.
232 he epidemics by placing the system below the percolation threshold.
233 n the mean-field result and to vanish at the percolation threshold.
234 stic strength being inversely related to the percolation threshold.
235 mals that contain enough metal to exceed the percolation threshold.
236 nch-off at melt fractions slightly below the percolation threshold.
237 fraction required to induce porous flow, the percolation threshold.
238 sional silver nanowire networks close at the percolation threshold.
239 permeability of static rock salt is due to a percolation threshold.
240 ed connection probabilities, approaching the percolation threshold.
241 ribed by a percolating system with different percolation thresholds for lipids and proteins.
242                           In general, static percolation thresholds may not always limit fluid flow i
243 ite percolation models in networks with null percolation thresholds, such as scale-free graphs with d
244 ical semiconductor (BSC) based on electrical percolation through a multilayer three-dimensional carbo
245 on, and presents a complete picture of O(2-) percolation through apatite.
246 inite element simulations to demonstrate how percolation through this actual 3D structure impedes ion
247  fluvial transport of nitrogen in rivers and percolation to groundwater accounts for approximately 35
248 ting topics, from geodesics in first-passage percolation to transit node-based route-finding algorith
249 sions-by employing analogies to the directed-percolation transition from nonequilibrium statistical p
250                                              Percolation transition produces porous nanocarbon with f
251                    We found that the Quantum Percolation Transition theory provides a better descript
252 dos-Renyi network formation model causes its percolation transition to become discontinuous.
253 ity can be associated to an abrupt bootstrap-percolation transition with cascades of extreme views th
254 uch lattices with small-world bonds, a novel percolation transition with explosive cluster growth can
255 onal insights on the anomalous nature of the percolation transition with null threshold.
256 in a network leads to the observation of the percolation transition, a structural change with the app
257 tive gap going to zero; and (b) as a Quantum Percolation Transition, where a sample-spanning metallic
258 governed by a random process often undergo a percolation transition, wherein around a critical point,
259                                      Whether percolation transitions could be discontinuous has been
260 am with two fundamentally different types of percolation transitions.
261 ence in a channel coincide with the directed percolation universality class.
262 acks at all packing densities through to the percolation value for this geometry, p(c) = 0.4072.
263 ich can be attributed to enhanced electrical percolation via the nonoxidized inner tubes.
264 d as oversimplified when the role of network percolation was included.
265                  Using the framework of link percolation we find that isolation increases the critica
266                The fate of melt water in the percolation zone is poorly constrained: some may travel
267 y the existing water storage capacity of the percolation zone of the Greenland ice sheet and show the
268 e increased surface melt is occurring in the percolation zone, a region of the accumulation area that
269 el rise will fill existing pore space of the percolation zone.

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