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1 olled nanoparticle assemblies in the form of colloidal particles.
2 ing aqueous solubility profiles in composite colloidal particles.
3 l double layer compression, similar to other colloidal particles.
4 in a suspension of synthetic photoactivated colloidal particles.
5 the entrapment in the biopolymeric matrix of colloidal particles.
6 s are nanoparticle assemblies in the form of colloidal particles.
7 tioning and thus enrichment of C(60)O in the colloidal particles.
8 repulsion that stabilizes bulk assemblies of colloidal particles.
9 entrifugation to shape-separate a mixture of colloidal particles.
10 lastic properties on the scale of individual colloidal particles.
11 tical sizing and mass density measurement of colloidal particles.
12 the control of specific DNA linkages between colloidal particles.
13 ectrochemical properties of alabandite (MnS) colloidal particles.
14 ectral region due to the periodic spacing of colloidal particles.
15 intracellular delivery of proteins and small colloidal particles.
16 ly suggests an analogy to the aggregation of colloidal particles.
17 of monodisperse, highly charged polystyrene colloidal particles.
18 tion somewhat like the Brownian movements of colloidal particles.
19 g such structures is through the assembly of colloidal particles.
20 n of anisotropic chainlike structures by the colloidal particles.
21 y for shape control of anisotropic polymeric colloidal particles.
22 es a new method for the directed assembly of colloidal particles.
23 deformation of a lipid membrane by adhering colloidal particles.
24 f the effective electrostatic forces between colloidal particles.
25 ding free DNA strands and DNA-functionalized colloidal particles.
26 a condensed matter analog, a 2D ensemble of colloidal particles.
27 olymer interface in densely polymer-tethered colloidal particles.
28 ining dense amorphous packings of core-shell colloidal particles.
29 s that are driven by changes in the shape of colloidal particles.
30 rd guiding interactions of biomolecules with colloidal particles.
31 application of a coupled resonance model for colloidal particle adhesion in a liquid phase theoretica
32 dynamically tune an assembly of anisotropic colloidal particles adsorbed at fluid-fluid interfaces u
34 ribution around a pair of such heated/cooled colloidal particles agrees quantitatively with the theor
35 olarized optical microscopy that anisotropic colloidal particles align perpendicular to the flow dire
37 developed to study the ionic interaction of colloidal particles and biopolymer molecules on a microa
38 , detection, and treatment, as well as novel colloidal particles and building blocks for mutlifunctio
39 ss made in the synthesis of nanocrystals and colloidal particles and draw analogies between these new
40 de a minimally invasive means for delivering colloidal particles and engineered red blood cells acros
41 itions, as demonstrated in recent studies of colloidal particles and glass-forming metallic systems.
42 ent, separation mechanism for mum and submum colloidal particles and organelles, taking advantage of
44 ability to manipulate small fluid droplets, colloidal particles and single cells with the precision
45 e interrelation between surface chemistry of colloidal particles and surface adsorption of biomolecul
46 se of attractive Coulomb interaction between colloidal particles and surfactant structures offers a p
48 thesis of the support in the presence of the colloidal particles, and (iii) direct impregnation of th
49 tags may be used to organize the assembly of colloidal particles, and DNA templates can direct the gr
50 ical composition, size and polydispersity of colloidal particles, and many methods have been develope
52 sma resonance, while those of semiconducting colloidal particles are determined by their size-depende
56 where the sodium borohydride-reduced silver colloidal particles are present, Stokes spectra collecte
57 ause the (111) planes of the fcc polystyrene colloidal particle array have an approximately 200-nm la
58 ), colloidal crystal templating (3-D ordered colloidal particles as a template), and super lattice ro
59 The newly formed interface sequesters the colloidal particles; as the interface coarsens, the part
61 roughput method can yield surface-structured colloidal particles at a rate of approximately 10(7) to
62 surements of attractive interactions between colloidal particles at an oil-water interface and show t
63 resent an experimental realization of patchy colloidal particles based on material independent deplet
64 py, respectively, reveal that 1-microm-sized colloidal particles bearing nuclear transport receptors
65 roach to the synthesis of asymmetric, hybrid colloidal particles by precipitation polymerization.
67 e diffusion rates of a wide range of natural colloidal particles can be predicted from theory, so lon
68 on reports that needle-like supercrystalline colloidal particles can be synthesized through anisotrop
70 mechanisms by which globular macromolecules (colloidal particles) can cause polymer-coated nanopores
71 of negatively charged surfaces (for example, colloidal particles) can spontaneously partition into an
72 microcapsules with shells of densely packed colloidal particles closer to application in fields such
73 picture describing their behavior is that of colloidal particles; colloids exhibit a sharp increase i
75 sis and functionalization of nanometer-sized colloidal particles consisting of well-defined, water-so
76 has been proposed that complex nonspherical colloidal particles could act as "colloidal molecules" i
78 n based formation of colloidal capsules, the colloidal particle deposition on (sacrificial) templates
79 rmed by the disclination loops that entangle colloidal particles dispersed in a nematic liquid crysta
82 of a theoretical phase diagram obtained for colloidal particles displaying short-range attractive in
84 wever, in other respects, the nonequilibrium colloidal particles do not behave as monopoles: They can
88 ave been developed to direct the assembly of colloidal particles, fabrication of crack-free and trans
89 ate the potential of these superparamagnetic colloidal particles for high-throughput analysis of glyc
90 ss of materials, namely colloidosomes (using colloidal particles for Pickering stabilization and fusi
91 have since exploited the Brownian motion of colloidal particles for studies of dissipative processes
93 scillatory micromotor system in which active colloidal particles form clusters, the size of which cha
94 ame size fraction-possibly due to release of colloidal particles from LSL corrosion scale enriched wi
101 res from primary building blocks (molecules, colloidal particles) has made remarkable progress over t
105 dynamic and optical scattering properties of colloidal particles having nonspherical morphologies.
106 bined with Maxwell's equations, suggest that colloidal particles heated or cooled in certain polar or
111 jums may lead to controlled self-assembly of colloidal particles in nematic and paranematic hosts, wh
112 m cations used in the reductive synthesis of colloidal particles in solution at room temperature.
113 the advantage of entrapping quercetin in the colloidal particles in terms of the chemical stability i
114 ation gradient to drive autonomous motion of colloidal particles in the highly confined space, and th
116 ported, obtained by frothing a suspension of colloidal particles in the presence of a small amount of
117 instant assembly of superparamagnetic (SPM) colloidal particles inside emulsion droplets of UV curab
123 at is capable of organizing a diverse set of colloidal particles into highly reproducible, rotational
124 the sole mechanism that enables transport of colloidal particles into or out of the channels, but it
128 he monopole-like fields around heated/cooled colloidal particles is crucial because the experimental
130 d transition in a 2D crystal of paramagnetic colloidal particles is induced by a magnetic field [Form
131 d assemble three-dimensional structures from colloidal particles is limited by the absence of specifi
133 substances--in particular macromolecules and colloidal particles--is a canonical problem limiting adv
136 putum greatly reduces the diffusion rates of colloidal particles, limiting the effectiveness of gene
138 omimetic, self-templating assembly of chiral colloidal particles (M13 phage) into functional material
139 y the method proposed here to real data from colloidal particles, microgels, and polymer solutions.
142 erated by the dissociation of carbonic acid, colloidal particles move either away from or towards the
144 trands is "stamped" from a gold surface onto colloidal particles of different sizes by streptavidin-b
150 sules are fabricated by the self-assembly of colloidal particles onto the interface of emulsion dropl
151 wnian dynamics of individual tracers such as colloidal particles or lipid domains have provided insig
155 ourants respectively and incorporated in the colloidal particles prepared from food protein-zein.
157 consequence of reduced crystallinity of the colloidal particles, presumably due to the different coo
159 pt of a jamming phase diagram for attractive colloidal particles, providing a unifying link between t
160 knotted nematic disclinations stabilized by colloidal particles raised a challenge of free-standing
161 nt evaporation, non-interacting monodisperse colloidal particles self-assemble into a close-packed su
163 serted interstitials in a lattice of similar colloidal particles sitting on flat or curved oil/glycer
167 heterotypic aggregation of cell mixtures or colloidal particles such as proteins occurs in a variety
168 sional reduced graphene oxide structures and colloidal particles, such as trefoil knots, with 'frozen
169 nating current (ac) electrokinetic motion of colloidal particles suspended in an aqueous medium and s
170 nk contains bubbles stabilized by attractive colloidal particles suspended in an aqueous solution.
171 is framework to the study of the dynamics of colloidal particle suspensions for packing fractions cor
173 o immiscible liquids, kinetically trapped by colloidal particles that are irreversibly bound to the o
174 ed nematic layers stabilized by 2D arrays of colloidal particles that can be controlled with laser tw
175 ed on a controlled deformation of multiphase colloidal particles that can be selectively liquified, p
176 f boojums by controlling surface topology of colloidal particles that impose tangential boundary cond
177 poly(N-isopropylacrylamide) (PNIPAM) nanogel colloidal particles that self-assemble into crystalline
178 h GO sheet is a single molecule as well as a colloidal particle, the molecule-colloid duality makes i
181 pect ratio of the asymmetric block copolymer colloidal particles to be correlated with the experiment
182 : during the deposition process, this causes colloidal particles to be swept from darkened areas into
183 LCA) to a multicomponent system of spherical colloidal particles to enable the rational design and pr
184 hat both models predict selective binding of colloidal particles to large target molecules on the sur
185 o diverse nucleation scenarios, ranging from colloidal particles to natural gas hydrates, and that, a
186 apillarity can be used to direct anisotropic colloidal particles to precise locations and to orient t
187 ed nematic liquid crystals (LCs) to assemble colloidal particles trapped at the LC interface into rec
188 An optical binding force between two nearby colloidal particles trapped by two coherent laser beams
190 neering thin magnetic films onto homogeneous colloidal particles, various crystalline lattices are in
191 ) pascals, containing high concentrations of colloidal particles (volume fraction phi greater, simila
194 ntropic ordering characteristics of athermal colloidal particles, we demonstrate that high-symmetry n
195 conjunction with the structural rigidity of colloidal particles, we demonstrate the parallel self-as
202 tudy the motion of asymmetric self-propelled colloidal particles which have a homogeneous mass densit
203 re solvent to be absorbed into the polymeric colloidal particle, which, in turn, lowers the glass tra
204 curs via the flocculation of semicrystalline colloidal particles, which results in the gels exhibitin
205 uid-to-solid transition of weakly attractive colloidal particles, which undergo markedly similar gela
206 non-aqueous suspension of 'sticky' polymeric colloidal particles with a controlled degree of polymeri
207 s colloidal spheres as keys and monodisperse colloidal particles with a spherical cavity as locks tha
208 e colloidal analogues of atoms with valence: colloidal particles with chemically distinct surface pat
213 ely 10(8)) of both non-magnetic and magnetic colloidal particles with micrometre precision and typica
214 rface active compounds lead to production of colloidal particles with more desirable physicochemical
215 methods offer scalable means of synthesizing colloidal particles with precisely specified size for ap
216 ructures of controlled size and shape out of colloidal particles with short-ranged interactions.
218 S20, SC and GA could produce the astaxanthin colloidal particles with small particle size, polydisper
223 relies upon the spatial organization of the colloidal particles within the polymer network that depe
224 merical determination of forces between such colloidal particles would be complicated by the presence
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