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1 o the low-density form at 130 K, but remains diffusive.
2 ng from the elongasome complex with the more diffusive action of aPBPs.
3  the size of proteins is too low to overcome diffusive action.
4                                              Diffusive-advection modelling demonstrates that low chlo
5  process in electronic devices, we developed diffusive Ag-in-oxide memristors with a temporal respons
6 ummer stratification, and at most 15% of the diffusive air-water-methane flux from the epilimnion.
7 oyed stents together with the combination of diffusive and advective drug transport render an intuiti
8 percooled and amorphous states, and of water diffusive and collective dynamics, in disparate thermody
9 mic chamber for the continuous monitoring of diffusive and ebullitive fluxes of methane (CH(4)) in aq
10 ntial reaction intermediates are collective, diffusive and of a molecular length scale.
11                                 We show that diffusive and superdiffusive types of motion are inheren
12 cally how the movement pattern that includes diffusive and superdiffusive/superballistic motion arise
13 between diffusive states or a combination of diffusive and transport states with opposite directional
14 ly controlled disorder to observe ballistic, diffusive, and arrested atomic transport.
15 ical states that include epochs of directed, diffusive, and stalled motion.
16 hm to classify switching between processive, diffusive, and stuck motility states.
17 ured substrates and can produce wafer-scale, diffusive, angle-independent, and flexible plasmonic mat
18  to intersite tunnelling, we instead observe diffusive atomic transport, signalling a crossover from
19 articles either aggregate near the magnet or diffusive away from the magnet, respectively.
20  thus may substitute for histology to reveal diffusive axonal injury pathologies in vivo.
21 suggest that the septin cytoskeleton forms a diffusive barrier around nascent podosomes to promote th
22  long-standing challenge owing to the strong diffusive barrier properties of the skin.
23 es a sulfur-impregnated carbon sorbent and a diffusive barrier.
24 that migration in these films is essentially diffusive because intrinsic chromophore energetic disord
25 fference with neat water, which demonstrates diffusive behavior (tau proportional, variant q(-2)).
26  as they navigate the pore space, exhibiting diffusive behavior at long time scales.
27          The applied model predicts a normal diffusive behavior at very short and long time lags, as
28  detected and localized temporary changes of diffusive behavior both in time and in space.
29 ver and the actin filament's resulting super-diffusive behavior in the actomyosin-cross-linker system
30 s from studies in vitro Comparisons with the diffusive behavior induced by the ribosome-binding antib
31                                    Thus, DDB diffusive behavior most likely results from dynein switc
32              Protein crowding alters the sub-diffusive behavior of proteins and lipids such as PIP2 w
33 provides an in-depth analysis of the complex diffusive behavior of RNA-protein particles in live cell
34 n polymerization and nuclear rigidity on the diffusive behavior of the nucleus.
35                    We describe the soliton's diffusive behavior using a quasi-1D scattering theory of
36           These bilayers exhibit a switch in diffusive behavior, becoming anomalous as bilayer contin
37 ed to other systems exhibiting non-Markovian diffusive behavior.
38 e observed diffusion is a complex mixture of diffusive behaviors (directed, Brownian, anomalous, or c
39 oxylated polystyrene NPs, we examined how NP diffusive behaviors change as a result of calcium-induce
40 me and related quantities and find different diffusive behaviors for different games.
41             We attribute the transient super-diffusive behaviour to the rapid expansion of the excite
42 tropic interactions (the XXX model), we find diffusive behaviour.
43 te-specific complex indicated that 1) freely diffusive binding by ETV6 proceeds through a nonspecific
44     Furthermore, we show that the concept of diffusive binding can also be utilized for the spatially
45 onic tracks that exploit Brownian motion and diffusive binding to transport cargo without using a che
46 xygen microelectrode recordings in the coral diffusive boundary layer revealed hyperoxia during dayti
47 ynamic changes in oxygen levels in the coral diffusive boundary layer, and the importance of fermenta
48 ction to that of O(2) , across the roots and diffusive boundary layer.
49  with minimal effects from biofouling or the diffusive boundary layer.
50   In this letter, we demonstrate that in the diffusive case, the conventional description of the insu
51                 Our approach yields a global diffusive CH(4) flux of 2-6TgCH(4)yr(-1) from the ocean
52                                          The diffusive character of both the high- and low-density fo
53 oscopic level, the hopping behavior leads to diffusive charge transport and is quantifiable as an app
54 to the cloak's interior), the sensitivity of diffusive cloaks to defects and approximations has not b
55 hold for the macroscopic drift behavior of a diffusive cluster or molecule physisorbed on a solid sur
56 aw predicts smaller cells to have a superior diffusive CO(2) supply.
57 he cloud, as if the system has turned into a diffusive collision-full classical system.
58  accelerated the electron transfer under low diffusive conditions.
59 le correlation between stomatal porosity (or diffusive conductance to water vapour g(s) ) and CO(2) a
60 n lead to significant errors when predicting diffusive contributions to flocculation and to single co
61 ion and thus mechanics of the layered C-S-H: diffusive-controlled and displacive-controlled deformati
62 viously identified and the associated double diffusive convection has been suggested to influence the
63 hallenge to understanding the role of double diffusive convection in vertical heat transport is one o
64 as those observed in the ocean due to double-diffusive convection.
65  relate the results quantitatively to double-diffusive convection.
66 ificantly increase in the presence of double diffusive convection.
67 work of generalized hydrodynamics, including diffusive corrections.
68                                              Diffusive coupling (calcein transmission) in vitro was s
69   The geometry of the traps controlled their diffusive coupling to fluid flow that played a dual role
70                 Depending on the strength of diffusive damping, the model exhibits complex growth pat
71  major interfacial component, and the reacto-diffusive depth of ozone in the triolein coating is esti
72 o exercise are minimized, the convective and diffusive determinants of VMO2peak , at the level of the
73 tion of the multivariable problem of kinetic-diffusive differential equations to a single variable pr
74                            Results show slow diffusive dislocation motion at nm/s inside ICNPs and fa
75 ovides insight into the atomic-scale coupled diffusive-displacive deformation mechanisms, maximizing
76 re, (b) the electrostatic force, and (c) the diffusive drag force that is a central feature of the Ma
77 computational finite element (FE) models for diffusive drug release from nanofibers to the three-dime
78          We find that the carriers exhibit a diffusive dynamics at times shorter than 200 ps, with a
79  analysis based on the Langevin equation for diffusive dynamics, which allows us to decompose errors
80 namics, and we consider systems described by diffusive dynamics.
81 ty that is the ratio between overlapping and diffusive effects.
82 s for an emergent electron gas that supports diffusive electrical transport.
83 g aspect of this search is that it relies on diffusive encounters with the crowded cellular backgroun
84 nversion was used to obtain the timescale of diffusive equilibration in spines and followed by global
85  of diffusive gradients in thin films (DGT), diffusive equilibration in thin films (DET) and the "DGT
86 ile the fundamental equations describing the diffusive equilibration processes, including a complemen
87                Experimentally, we found that diffusive equilibration was often slower, but rarely fas
88 used to assess the role of morphology on the diffusive equilibration.
89 ter designed for fungus was adapted here for diffusive equilibrium in thin film gel techniques (DET).
90 A novel methodology is presented here, using Diffusive Equilibrium in Thin-film (DET) gels as high-sp
91 plained by the combined influences of random diffusive error and systematic drift toward a set of sta
92 s along a single pathway, corresponding to a diffusive escape process across a free energy barrier.
93                  After the three-dimensional diffusive escape process, a one-dimensional diffusive re
94 ect bubble transport (0-2 kt yr(-1)) and via diffusive exchange of methane dissolving in the surface
95 operties suggested that the atmosphere-ocean diffusive exchange of OPEs could be 2-3 orders of magnit
96 ryonic body and a one-compartment model with diffusive exchange were calculated for the neutral test
97 , such as self-trapped localized motion, 2-D diffusive exploration, and super-diffusive persistent mo
98 hange between stably clustered and laterally diffusive extra-clustered channels maintains steady-stat
99 ight, M(w), we report the emergence of a new diffusive "fast" relaxation mode at higher values of C(p
100 gomers can lead to significant shifts in the diffusive features and recapitulate the modifications ob
101  that PL transport can occur via a high-flux diffusive flow mechanism.
102                             An overestimated diffusive flux and underestimated permeability are obtai
103 s for the continuous quantification of CH(4) diffusive flux higher than 25 x 10(-6) g m(-2) h(-1), th
104  This is the first report of vapor phase and diffusive flux of both PAHs and OPAHs during the DWH.
105              Pores nevertheless allow a high diffusive flux of more than 66 molecules per second that
106 unoff reaches the ice margin, with estimated diffusive fluxes (4.4 to 28 millimoles of CH(4) per squa
107                    Calculated sediment-water diffusive fluxes greatly overwhelmed the atmospheric dep
108 tive but allowed for the characterization of diffusive fluxes higher than 10 mg CO(2) m(-2) h(-1) and
109                                Comparison of diffusive fluxes of nuclear probes between wild-type and
110 r soil water propagation, heat transfer, and diffusive gas transport to explain observed soil moistur
111       By using a combined planar optode-DGT (diffusive gradient in thin-films) sensor we obtained sim
112                   The analytical techniques, diffusive gradients in thin films (DGT) and Chelex colum
113                                              Diffusive Gradients in Thin Films (DGT) devices can meas
114                                          The diffusive gradients in thin films (DGT) passive sampling
115 drogel sensing layer was integrated with the diffusive gradients in thin films (DGT) technique for th
116      The in situ passive sampling technique, diffusive gradients in thin films (DGT), confronts many
117                          The combined use of diffusive gradients in thin films (DGT), diffusive equil
118 tu passive sampling techniques, such as the "diffusive gradients in thin films" (DGT) technique, prov
119     This mobilization was studied using DGT (diffusive gradients in thin films): vertical one-dimensi
120 essment in Antarctic marine conditions using diffusive gradients in thin-films (DGT) coupled to regio
121             The passive sampling approach of diffusive gradients in thin-films (DGT) is developed her
122 luated in 10 agricultural UK soils using the diffusive gradients in thin-films (DGT) technique.
123               The passive sampling method of diffusive gradients in thin-films (DGT) was developed to
124 opulation sizes slow, characterised by a sub-diffusive growth law; 2) the molecular phenotypes under
125 f, and find a quadratic relation between the diffusive half-time and the averaged mean curvature of t
126                             We determine the diffusive half-time, i.e., the time that is required to
127 de evidence for a strongly elevated vertical diffusive heat flux across the base of the mixed layer i
128 mplers containing synthetic FeOx embedded in diffusive hydrogels.
129                    The results show that the diffusive in-cell motions, after all, follow simplistic
130                       In contrast, the term 'diffusive' is more akin to a chaotic propagation in scat
131 he polaron propagates through the crystal by diffusive jumps over several lattice spacings at a time
132  reproducing material-level, dissipative and diffusive kinetic phenomena at the structural level, whi
133 and stretched exponential model-derived mean diffusive length scale (Lm(D)) from DW MRI was compared
134 Helium 3 diffusion-weighted MRI-derived mean diffusive length scale demonstrates longitudinal changes
135 dynamics demonstrates that refocusing of the diffusive light is based on ~15-ps initial dipole moment
136 ion enhances random displacements to amplify diffusive-like motion.
137 ure of bond-based interactions facilitates a diffusive-like re-orientation of the parasite at the RBC
138                                       In the diffusive limit, the particle concentration is linearly
139 capable of describing such a scenario in the diffusive limit, we consider the emergent physics in hyb
140 stics in Bi0.96Sb0.04 single crystals in the diffusive limit, which occurs only for a magnetic-field-
141                              Biochemical and diffusive limitations to leaf photosynthetic CO(2) uptak
142 lso reveals previously unknown ballistic and diffusive limits for magnetophoresis wherein the paramag
143 d to lead to thermalization and conventional diffusive linear response.
144 et by the balance between the resistances to diffusive loading from the source and convective export
145 loading is nearly length-independent, unlike diffusive loading, which is biased towards shorter fragm
146             Finally, buffer exchange reduces diffusive losses and band broadening, even when handling
147 tially impacts analytical sensitivity due to diffusive losses of protein out of the open microfluidic
148        In this study, a site-specific stress-diffusive manipulation is demonstrated to fulfill highly
149 s of REEs separation via LEM were limited by diffusive mass transfer across the liquid membrane.
150                     Exact calculation of the diffusive mean first-passage time on a spatial network i
151  the extracellular distribution of Wnt3 by a diffusive mechanism that is modified by tissue morpholog
152             To exploit the underlying stress-diffusive mechanism, a physical model is provided by usi
153 that Mec1 primarily uses a three-dimensional diffusive mechanism, whereas Tel1 undergoes directed mot
154  microtubule lattice in combination with the diffusive mechanochemical cycle of the motor.
155 settings such as around corners, and through diffusive media.
156                                          The diffusive memristor and its dynamics enable a direct emu
157             The random bits generated by the diffusive memristor true random number generator pass al
158                Here we demonstrate a type of diffusive memristor, fabricated from the protein nanowir
159 lay time of threshold switching in a Ag:SiO2 diffusive memristor, which exhibits evident advantages i
160                  Remarkably, the barriers to diffusive menaquinone dynamics are lesser than that of t
161 l developed for wave systems, the studies of diffusive metamaterials have been limited by their chara
162 The relative distributions of persistent and diffusive migration can be changed by modification of th
163 dendritic cells move along curved paths, and diffusive migration, which is characterized by successiv
164 P converts MutS to a hydrolysis-independent, diffusive mobile clamp that no longer recognizes the mis
165                            Notably, a strong diffusive mode around zero frequency arises, which is no
166 ot possibly exceed 1 for any one-dimensional diffusive model, no matter how rugged its underlying fre
167 table localization microscopy to observe the diffusive modes of Lck in the plasma membrane.
168 ause its imaging power derives entirely from diffusive molecular dynamics, DNA microscopy constitutes
169 racted to their conspecific female gamete by diffusive molecules, called chemoattractants, released f
170 ntaneous formation of ssDNA bulges and their diffusive motion along SSB surface was directly observed
171 en bulk flow to dominate over random thermal diffusive motion at the scale of a single eukaryotic cel
172    HS-AFM data reveal that the CNTPs undergo diffusive motion in the bilayer plane.
173    We also found that without solvation, the diffusive motion is quenched.
174                                          The diffusive motion of a subset of ribosomes is also frozen
175 correlations of DNA in DNA arrays as well as diffusive motion of DNA and cations.
176 efore, PTCH1 inactivation by SHH changes the diffusive motion of PTCH1, possibly by modifying the mem
177 TP(t) from theories assuming one-dimensional diffusive motion over a harmonic barrier.
178 in which the domain's free state undergoes a diffusive motion that is quenched in the bound state, li
179                  Importantly, SVs exhibiting diffusive motion were relatively less likely to switch t
180 ontaneous symmetry breaking, short-timescale diffusive motion, and spontaneous cell-motion reorientat
181 e skeleton that may occur via anchor protein diffusive motion, that is, band 3 and glycophorin, throu
182 s a minority number of them had active super-diffusive motions driven by motor proteins.
183  The single-headed form of KIF1A is a highly diffusive motor that has been shown to be a prototype of
184 l trapping data, suggesting that the motors' diffusive movements on the vesicle surface and the exten
185  is known about other transport regimes like diffusive multiple scattering or Anderson localization.
186 inant models of MMR initiation that envision diffusive MutS-MutL complexes that move away from the mi
187                                   Due to the diffusive nature of thermal energy, thermal insulation i
188 ral frontoparietal mechanisms in response to diffusive noise and of stimulus-specific biases in occip
189        This transformation is neither purely diffusive nor purely martensitic as conventionally assum
190  or near dislocations markedly transform the diffusive nucleation with an intermediate-stage liquid i
191 id-solid transitions between crystals follow diffusive nucleation, or various diffusionless transitio
192 cillation of dislocation pairs followed by a diffusive nucleus growth.
193                  The estimated vertical eddy diffusive nutrient fluxes across diapycnal surfaces reac
194 69 +/- 0.07 l min(-1) , P < 0.05) and muscle diffusive O(2) conductance (6.6 +/- 0.8 vs.
195 ats due, in part, to impaired convective and diffusive O(2) delivery, and thus V O(2) , especially wi
196 hosphorescence quenching) and convective and diffusive O(2) transport ( Q O(2) and DO(2) , respective
197 organization of the point-to-point electric, diffusive or hydraulic transport in complex scale-free n
198 oiling dissipation (the latter may either be diffusive or mediated by topological enzymes, such as ty
199  to whether animal movement is predominantly diffusive or superdiffusive has been a focus of discussi
200 ctures that combine reflective, diffractive, diffusive, or absorbing domains.
201 hibit as either acoustic (resonance) mode or diffusive (overdamped) mode.
202 s was tested that both muscle convective and diffusive oxygen (O(2) ) transport, and therefore skelet
203 letal muscle microvasculature and subsequent diffusive oxygen delivery to the mitochondria were dimin
204                                              Diffusive oxygen shunting plays a significant role in th
205 tive contribution from the channeled and the diffusive paths depends on the overlap between the off-r
206 ngs demonstrate the existence of a high-flux diffusive pathway for PL flow in Escherichia coli that i
207 th certain probability, along a few dominant diffusive pathways.
208 etabolite compartmentation, biochemistry and diffusive pathways.
209 hip models, however, is typically limited to diffusive permeability measurements that are exclusively
210 motion, 2-D diffusive exploration, and super-diffusive persistent motion.
211 horetic regime that is ballistic rather than diffusive, persisting up to and beyond a 100-nanometer s
212 gs demonstrate the benefits of anomalous sub-diffusive photon transport in active media with correlat
213 against well-established electrophoretic and diffusive processes and differ for each.
214      Estimates of Ohmic heating suggest that diffusive processes likely govern the ultimate decay of
215  importance membrane geometry plays in these diffusive processes, it is challenging to establish the
216 u (EF-Tu), and DNA spatial distributions and diffusive properties in intact Escherichia coli cells.
217                                          The diffusive properties of EF-Tu remain quantitatively indi
218  free-rider co-evolution in the context of a diffusive public good (PG) that is produced by the produ
219  that single and pairs of cells migrate as a diffusive random walk for at least 7 hours of evolution.
220 h to employ the theoretical framework of the diffusive random walk for the prognostic modelling and o
221  1,2-propanediol substrate concentration and diffusive rates, on when active transport of the substra
222  on dextran size in a manner consistent with diffusive rather than convective transport; (ii) transpo
223 rved changes in lipid composition are due to diffusive rather than localized effects on TNF-alpha pro
224   A dynamic equilibrium between anchored and diffusive receptors is a common feature among ion channe
225  diffusive escape process, a one-dimensional diffusive regime describes on rates.
226 nteraction phenomena beyond the conventional diffusive regime.
227  intervals, cells exhibit an additional fast diffusive regime.
228 l movement transitions from a ballistic to a diffusive regime.
229 lowing DNA damage, DNA exhibits distinct sub-diffusive regimes.
230 ng the competition between shear banding and diffusive relaxation processes, and is reminiscent of th
231 aling speed of simple diffusion by utilizing diffusive relays, in which the presence of one type of d
232  analysis shows these tumbles cause in-plane diffusive reorientations with 1.5 rad(2)/s rotational di
233         We have previously proposed that the diffusive return of the kinesin motor that powers intraf
234      A full transition from the conventional diffusive rotation to superdiffusive rotation and furthe
235 d through ultrafast electron diffraction and diffusive scattering techniques with varying excitation
236 d approximately 1,900 times greater than the diffusive sea-air methane efflux (17.3 +/- 4.8 mumol m(-
237 pping on actin filaments, executing a random diffusive search for actin binding sites at each step.
238                               We investigate diffusive search on planar networks, motivated by tubula
239 ange, regulate transcription, and facilitate diffusive search processes.
240 A stochastic sequence of processive runs and diffusive searches results in a biased random walk.
241 iangular pore-aperture driving the efficient diffusive separation of propylene from propane in mixed-
242 ose a new paradigm for polarity formation: A diffusive signal triggers cell polarization by promoting
243 bed by a dimensionless number accounting for diffusive soil creep, runoff erosion, and tectonic uplif
244 lic conductivity, reflection coefficient and diffusive solute permeability).
245                              We observed two diffusive species: fast (with a diffusion coefficient of
246                                 The observed diffusive spin excitation persists at the lowest measure
247                      The combination of this diffusive spin torque and the spin-orbit torque results
248 beginning and eventually slowing down to the diffusive spread [Formula: see text].
249 pe complexity of the membrane influences the diffusive spreading of proteins and molecules.
250            A possible hypothesis is that the diffusive state enables the motor to explore the microtu
251 ing phosphorylation at Ser-1700 promoted the diffusive state of CaV1.2 irrespective of the differenti
252  depletion, the molecules that remain in the diffusive state showed a significant increase in the dif
253 revalent diffusive states, the timescales of diffusive state switching can be determined by stepwise
254 a Brownian motor by virtue of a weakly bound diffusive state to the microtubule.
255 ment with the shift of isolated DDB into the diffusive state.
256 ults from dynein switching into an inactive (diffusive) state, rather than p150 tethering the complex
257    Here, we show that multiple intracellular diffusive states can be successfully resolved if suffici
258 KRAS4b exhibits confined mobility with three diffusive states distinct from the other RAS isoforms (K
259 deling, we found that SVs oscillated between diffusive states or a combination of diffusive and trans
260 g to accurately resolve and characterize the diffusive states that can manifest in the cytosol using
261 on coefficients and populations of prevalent diffusive states, the timescales of diffusive state swit
262 d to classify BCR trajectories into distinct diffusive states.
263  environment, a combination of ballistic and diffusive steps is considered optimal; in particular, mo
264 ics place this form of the oxide in a highly diffusive, strong disorder regime and establishes the ex
265 limit in using molecular networks to harvest diffusive sun photons on large areas and funnel them ont
266 selective pressures associated with improved diffusive supply of the terrestrial environment.
267 he emergence of traveling patterns in purely diffusive systems with conservative dynamics.
268             Instead, for static E. coli, the diffusive T4 mutant lacking Ig domains outperformed the
269 ynein processivity not solely by acting as a diffusive tether that maintains microtubule association,
270             In the normal state we observe a diffusive thermal conductivity that is approximately tem
271       Here we observe that for these systems diffusive thermal transport is controlled by a universal
272  manner, providing atomistic resolution over diffusive time scales using no adjustable parameters.
273 ndings thus help estimate the characteristic diffusive timescale based on the simple measure of membr
274 d changes to hemoglobin concentration (i.e., diffusive tortuosity) and cell size (i.e., diffusion pat
275 e-step displacements from ribosome and EF-Tu diffusive trajectories before and after Onc112 treatment
276 cal impedance spectroscopy demonstrated that diffusive transport accelerates.
277 ng evaluates drug vascular extravasation and diffusive transport as key RF-modulated parameters, with
278             Results show that RF facilitates diffusive transport in 3D cell cultures representing hyp
279 conds and 600 nanometers before reaching the diffusive transport limit.
280 es, and accurately described by a convective-diffusive transport model, provided a means to calculate
281 that the evaporation results from the purely diffusive transport of liquid vapor and that the contact
282 , however, the performance is limited by the diffusive transport of target molecules to the surface.
283 onstrating the importance of the tail in the diffusive transport of these viruses.
284  epsilon is due to a two-step process, where diffusive transport of U(VI) from the bulk solution acro
285 articles in the CSF via a coupled convective-diffusive transport process.
286 y factor quantifies the apparent decrease in diffusive transport resulting from convolutions of the f
287 ture dependence can also be caused by highly diffusive transport that, in highly disordered materials
288 apid clearance from the joint space and slow diffusive transport through the dense, avascular cartila
289 tions, accompanied by the onset of anomalous diffusive transport throughout the system, and verify th
290 -dimensional model was developed to simulate diffusive transport, abiotic and biotic transformation,
291 duct) interaction with the pore surface, and diffusive transport.
292 ossover in the time domain from ballistic to diffusive transport.
293  due to thermionic emission rather than bulk diffusive transport.
294 S can be used to reconstruct the flux (i.e., diffusive vs. advective) and timing of CH(4) emissions i
295 of their phases and the complex interplay of diffusive vs. displacive phase transformations to permit
296 rate time scales of motion, corresponding to diffusive water (DW) and protein-water coupled motions,
297 llective effect gives rise to fast-traveling diffusive waves.
298 es, we find that cell trajectories are super-diffusive, where displacements scale faster than t1/2 in
299  of the molecular motion in the cytoplasm is diffusive, which possibly limits the tempo of processes.
300 2 mineralization, which will likely occur in diffusive zones adjacent to flow paths or in dead-end fr

 
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