ライフサイエンスコーパス: colloid

1 tania nanoparticles (as prototypical mineral colloids).

2 III), which then re-oxidizes yielding Pu(IV) colloid.

3 rt significant Pu chelation character to the colloid.

4 s between various components within this bio-colloid.

5 e based on the ratio of sampling air to SERS colloid.

6 but also for enriching the application of Au colloids.

7 s observed between the 140 and 200 degrees C colloids.

8 e detected as changes in the velocity of the colloids.

9 nteraction and weak diffusion for microscale colloids.

10 uid crystals or chemically engineered motile colloids.

11 arge, nonreactive building blocks such as Au colloids.

12 ing the self-assembly of materials made from colloids.

13 racemic colloidal superstructures in nematic colloids.

14 llagen, quantum dots, silver and polystyrene colloids.

15 nctional application for the conventional 2D colloids.

16 el crystallization pathways using DNA-coated colloids.

17 significantly affecting the mobility of the colloids.

18 ngth liberated significant concentrations of colloids.

19 d surface energy gradients for the diffusing colloids.

20 s composed of active and passive mixtures of colloids.

21 onventional test strip based on colored gold-colloids.

22 fraction of active (spinning) ferromagnetic colloids.

23 water interface of complex multiphase liquid colloids.

24 s inaccessible to micron- or nanometer-scale colloids.

25 gle spin-coating step from ultraconcentrated colloids.

26 ional Security Site (NNSS) and attributed to colloids.

27 ogical structure of subvisible particles and colloids (0.01-10 mum) in the supernatant of a lab-scale

28 ane foulants were dominated by particles and colloids (0.45-10 mum), which accounted for over 90% of

29 contained more live cells compared with the colloids (100 kDa-1 mum).

30 y conditions, have been demonstrated in such colloids(21-23).

31 or the sorption of 65% of PBDEs, followed by colloids (30%); only 5% of PDBEs were truly dissolved.

32 In liquid-crystal colloids(5-7), elastic interactions between particles ar

33 reliable as the gold-standard (99m)Tc-sulfur colloid ((99m)Tc-SC) for gastric emptying scintigraphy (

34 ikely including dissolved U and very small U colloids; a 1-3 kDa fraction containing humic-like organ

35 % CI, 1.02-1.05) and potentially modifiable (colloid administration [yes vs no]: OR, 1.75, 95% CI, 1.

36 Au/Ag colloids aggregated with simple salts are amongst the mo

37 a homogeneous pore space and largely ignore colloid aggregation.

38 tric responses of the two hemispheres of the colloids allow simultaneous control of particle motility

39 mproved by self-propelling or activating the colloids along the axis connecting their hydrophobic hem

40 plasma FT4 and TT4, and depleted follicular colloid and increased epithelial cell height at 18 days,

41 groundwater (1.8 mg/L) suggest that the high colloid and Pu concentrations observed in our 140 and 20

42 od tracers for the hydrological transport of colloids and (pathogenic) viruses.

43 is of light propagation in highly scattering colloids and biological samples.

44 Herein, we retrospect the history of 2D colloids and discuss about the concept of 2D nanomateria

45 th both promoted the mobilization of natural colloids and enhanced the transport of previously adsorb

46 ecause yeast autolysis enriches the wines in colloids and improves their effervescence, foam and arom

47 ogy-dependent fluorescence of complex liquid colloids and investigate the interplay between GFPc surf

48 cant role in the detachment and transport of colloids and microorganisms in confined systems as well

49 al surface architectures composed of complex colloids and nanoparticles as well.

50 based on the controlled synthesis of polymer colloids and optimization over the carbonization process

51 Persistent colloids and slow sustained ion release may have importa

52 4A in Colloids and Surfaces B: Biointerfaces, Volume 142, 1 Ju

53 , the desorption rates for the 140 degrees C colloids and the Pu-montmorillonite colloids were simila

54 ties will be closely tied with the nature of colloids and their hierarchical assemblies.

55 f materials, such as metal alloys, inorganic colloids and various types of soft matter.

56 We present a novel class of functional colloids and zeolite-based photonic crystals with the ab

57 ication (bulk soil --> crude colloid --> IEF colloid) and coincided with the trend of Pu concentratio

58 t vasopressor, and avoidance of starch-based colloids) and assessed their role in mediation of case v

59 locity in the vicinity of the surface of the colloid, and confirm a mechanism for propulsion that was

60 changes in the solution where breaking up of colloids, and a change in the solvent strength, leads to

61 ers composed primarily of passive (inactive) colloids, and a very small fraction of active (spinning)

62 lines in high-T (c) superconductors, charged colloids, and grain transport in eroded sand beds.

63 rials, especially in the form of soft matter colloids, and is one of the first demonstrations of succ

64 beyond the more familiar realm of polymers, colloids, and magnetic materials that all exhibit therma

65 ong effort about the whole development of 2D colloids, and plots a clear roadmap - "lamellar solid -

66 f nanoparticle vesicles from polymer-grafted colloids, and the closely related field of nanoparticle

67 observed in assemblies of interacting active colloids, and the theoretical tools that have been used

68 These colloids appear to provide nucleation sites for the pero

69 Active colloids are a class of microparticles that 'swim' throu

70 Brownian dynamics simulations that, when the colloids are attached to long semiflexible filaments, th

71 Gold (Au) colloids are becoming ubiquitous across biomedical engin

72 Consequently, ligand-free colloids are ideal reference materials for evaluating th

73 The latex monodisperse polystyrene (PS) colloids are important for different advanced applicatio

74 Colloids are mainly divided into two types defined by si

75 The resulting boroxine-linked colloids are the next class of 2D COFs to be obtained as

76 Colloids are ubiquitous in biological, chemical and tech

77 oscopic systems, elastic deformations of the colloids are usually disregarded due to the damping impo

78 Micron-scale colloids are widely used as model systems to study phase

79 ritical for the obtainment of stable polymer colloids as carbon precursors.

80 , such as in separation and fractionation of colloids, as well as in fundamental soft condensed matte

81 Recent advances in colloids assembly have been achieved by exploiting the m

82 ve implications for the release of colloids, colloid-associated contaminants, and pathogens from soil

83 However, formation of colloid-associated Pu will tend to decrease with time as

84 to the known attractive glass line of sticky colloids at low attraction strengths and extends it to h

85 well as the organization and dynamics of the colloids at the vesicle surface.

86 revealed that roughness decreases the gap in colloid attachment between favorable (repulsion absent)

87 ervations elucidate the role of roughness in colloid attachment under both favorable and unfavorable

88 anoscale heterogeneity dramatically enhances colloid attachment, and multiple interactions among aspe

89 resolution imaging and temporal evolution of colloid Au nanoparticles are recorded.

90 unting for patient morphometry, crystalloid, colloid, blood products, urine, blood loss, duration, an

91 osite response of migration of dissolved and colloid-bound tetracycline to the change in solution ion

92 cients that produced experimentally observed colloid breakthrough-elution concentration histories and

93 that hydrodynamic slip moderately decreases colloid bulk delivery, nanoscale heterogeneity dramatica

94 les (free amino acids, proteins and glucidic colloids), but the effect of temperature was more import

95 oute to obtain salt-free intrinsic plutonium colloids by ultrasonic treatment of PuO2 suspensions in

96 = Cs or methylammonium (MA)) type perovskite colloids (ca. 2-100 nm) can selectively photocatalyze ca

97 oids (ca. 9-16%) than from the 200 degrees C colloids (ca. 4-8%).

98 lutonium was desorbed from the 140 degrees C colloids (ca. 9-16%) than from the 200 degrees C colloid

99 Moreover, we show these active colloids can act as nucleation sites, and switch rapidly

100 ndeed, the facet contacts between ice and Au colloids can be better than the point-like counterparts

101 In general, hydrolytic and sonochemical Pu colloids can be described as core-shell nanoparticles co

102 f bovine serum albumin (BSA) to aqueous gold colloids can be quantified with molecular resolution by

103 ow that the motion of active, self-propelled colloids can be sufficiently controlled for use as a too

104 These AF(G)P-inspired Au colloids can directly adsorb onto a growing ice crystal

105 The stability of such colloids cannot be explained by traditional electrostati

106 conditions attachment increased via reduced colloid-collector repulsion (reduced radius of curvature

107 indings have implications for the release of colloids, colloid-associated contaminants, and pathogens

108 Colloids composed of inorganic particles in inorganic me

109 class of dynamically reconfigurable complex colloids comprising immiscible liquid crystals (LCs) and

110 d compared the resulting changes in effluent colloid concentration through multiple sampling ports.

111 Here, a direct link between the colloids concentration present in the [HC(NH2 )2 ]0.83 C

112 Furthermore, median colloid concentrations in NNSS groundwater (1.8 mg/L) su

113 At 200 degrees C, maximum Pu and colloid concentrations of 30 Bq/L and 150 mg/L, respecti

114 However, much lower Pu and colloid concentrations were observed at 25 and 80 degree

115 Self-propelled colloids constitute an important class of intrinsically

116 that bacterial cells in/on the particles and colloids could have an important effect on fouling in SA

117 ed decreased attachment being due to reduced colloid delivery rather than decreased attraction.

118 Colloid deposition in granular media is relevant to nume

119 teractions per asperity and asperity height; colloid detachment simulations were highly sensitive to

120 rium driving forces in a bacterial bath, the colloids disperse if disorder is added to the potential.

121 asting distances across which nonexponential colloid distribution from the source occurred in the fin

122 sition from hyperexponential to nonmonotonic colloid distributions from the source as driven accumula

123 n concentration histories and nonexponential colloid distributions from the source.

124 Colloids drive much current research owing to their dist

125 e establish first-passage-time symmetries of colloids driven by femtoNewton forces in holographically

126 s driven accumulation of mobile near-surface colloids due to relatively strong secondary minimum inte

127 the in situ movement of the antifreezing Au colloids during ice growth/recrystallization and clearly

128 dielectrophoretic "electric bottle" confines colloids, enabling precise control of the motion of the

129 y types and sizes (dimers, n-mers, micelles, colloids, etc.), each having their own unique properties

130 The smallest colloids exert a disproportionately large influence on c

131 at each LC interface, we prepare LC complex colloids exhibiting different internal configurations.

132 igration has been observed and attributed to colloid facilitated transport.

133 ntration in the effluent suggested that soil colloids facilitated the release of AgNP (cotransport).

134 bed on colloids) from ~4% to 30-40%, and the colloid-facilitated effect was larger at lower ionic str

135 This may give rise to more extensive colloid-facilitated transport and help explain why trace

136 To better understand the mechanism(s) of colloid-facilitated transport at this site, we performed

137 Such colloid-facilitated transport can be induced by changes

138 as size exclusion, has been responsible for colloid-facilitated transport of groundwater contaminant

139 However, colloid-facilitated transport played only a minor role i

140 bio-solutions where conventional aggregated colloids fail.

141 drus-PhreeqC) with the DLVO theory, extended colloid filtration theory and colloid release model.

142 anoparticles) and fluorophore-functionalized colloids (fluorescent polymer microparticles, dye-labele

143 roduce a previously undiscovered usage of Au colloids for advancing cryoprotectants with significant

144 t in segregated membranes, the soft microgel colloids form closely packed 2D crystals on the fluid bi

145 samples collected from the run 13-05 of the Colloid Formation and Migration (CFM) experiment at the

146 ne of the Grimsel Test Site (GTS) within the Colloid Formation and Migration (CFM) project.

147 ticular, emphasizes roles for desorption and colloid formation in its mobilization.

148 ation exchange) is not similarly affected by colloid formation temperature.

149 ultrasound contribute to the mechanism of Pu colloid formation.

150 ter in wastewater streams, stabilizes silver colloids from agglomeration in high salinity marine wate

151 through of ciprofloxacin (over 90% sorbed on colloids) from ~4% to 30-40%, and the colloid-facilitate

152 ed that the adhesion energy between a silica colloid glued to AFM cantilever and the studied surfaces

153 ression of purification (bulk soil --> crude colloid --> IEF colloid) and coincided with the trend of

154 hrocytes or historically with (99m)Tc-sulfur colloid has been a clinically useful tool since the 1970

155 tal-organic frameworks (MOFs) in the form of colloids has brought a paradigm shift in the design of n

156 ly, we highlight how formulation of ZIF-8 as colloids has led to the emergence of novel physicochemic

157 sms at stake in the propulsion of asymmetric colloids have been the subject of debates during the pas

158 Complex liquid colloids hold great promise as transducers in sensing ap

159 nated from the exotic plasmonic effect of Au colloids (i.e., localized surface plasmon resonance (LSP

160 The defect structure associated with a colloid in a nematic liquid crystal is dictated by molec

161 A silver colloid in the collection medium was used as the SERS ad

162 Attaining thermodynamic stability of colloids in a broad range of concentrations has long bee

163 how this exchange can affect the release of colloids in a soil are unclear.

164 behavior during bio- and photodegradation of colloids in boreal Fe- and DOM-rich humic waters (a stre

165 d crystals offers the capability to organize colloids in certain regions such as the cores of the top

166 ath was obviated by the use of nonbiological colloids in column transport experiments conducted in re

167 Transport of colloids in dead-end channels is involved in widespread

168 d for applications of inorganic nanoparticle colloids in optics, biology, and energy, their surface c

169 s a guide for researchers seeking to analyze colloids in this smallest size range using AF4-ICPMS wit

170 nductors and magnetic materials) form stable colloids in various molten inorganic salts.

171 On the micrometre scale, however, colloids in water defy the intuitively simple idea of fo

172 rlying the formation of such imine-based COF colloids in water.

173 ehaviors of nanoparticles and microplastics (colloids) in environmental granular media is an active a

174 scopic experiments reveal that microorganism-colloid interactions are dominated by rare close encount

175 Colloid Interface Sci.

176 hat describe the spontaneous organization of colloids into materials.

177 indicated that oxygen state in hydrolytic Pu colloid is influenced by hydrolysed Pu(IV) species to a

178 and nematic (I + N) coexistence for rod-like colloids is a signature of the first-order thermodynamic

179 Here, the optimum arrangement of charged colloids is experimentally investigated by encapsulating

180 Fundamental knowledge on intrinsic plutonium colloids is important for the prediction of plutonium be

181 f micrometre- and submicrometre-sized patchy colloids is now efficient, but surface patterning of ino

182 This dual effect of colloids is primarily due to the opposite response of mi

183 tility and immense practical utility of such colloids is showcased by the single NC spectroscopy on u

184 nscreened surface charge of LSPC-synthesized colloids is the key to achieving colloidal stability and

185 Since the feasibility of g-C3N4 aqueous colloids is well-established, g-C3N4 can be viewed as an

186 ncentrated far more than suspensions of hard colloids, leading to their unusual mechanical properties

187 ntaneously oligomerizes to form a metastable colloid-like suspension.

188 Within the catchment, humic colloids lost up to 50% of their copper-binding capacity

189 itu planned for standard radioactive-labeled colloid LSG with subsequent SLNB were randomly assigned

190 velopment, laser synthesis and processing of colloids (LSPC) has emerged as a convenient and scalable

191 of-care modified Brooke (MB), limited-volume colloid (LV-Co), and limited-volume crystalloid (LV-Cr)

192 both exceed the predictions from widely used colloid models.

193 The results for BSA on gold colloid nanoparticles can be modeled in terms of Langmui

194 the sodium adsorption ratio, (ii) extracting colloids/NPs from the soil matrix using sonication and a

195 uilibrium partitioning between particles and colloids: OC + BC were responsible for the sorption of 6

196 r, bio- and photodegradation of organoferric colloids, occurring within a few days of exposure time,

197 e dipolar nanoparticle tip from a core-shell colloid of Au@Co.

198 These dynamic LC complex colloids of controllable morphology and LC orientation a

199 Creating colloids of liquid metal with tailored dimensions has be

200 We have observed that the colloids of NaEu(CO3)2.nH2O formed in seawater are taken

201 d gap was similar for biogenic and synthetic colloids of similar size, but decreased when the enzyme

202 The adsorption of Fe colloids onto heterotrophic bacteria Pseudomonas aureofa

203 The stabilized colloids' optical properties were studied through optica

204 Stabilizing colloids or nanoparticles in solution involves a fine ba

205 active media, such as suspensions of active colloids or swimming microorganisms(2), differs consider

206 Colloid osmotic pressure (bolus resuscitation: 19.3 +/-

207 Here I review colloid osmotic pressure as a crowding metric.

208 ssure-tension model for nuclear shape, where colloid osmotic pressure generated by nuclear protein im

209 I discuss measurements of colloid osmotic pressure inside cells using the nucleus,

210 ma membrane cation permeability, followed by colloid-osmotic swelling.

211 ight scattering analysis, the dissolution of colloids over a time span triggered by the addition of h

212 The colloid particles first attract each other to form clust

213 spectrometry allowed the characterization of colloid populations and the determination of the size di

214 y used to separate nanoparticles from larger colloids prior to analysis (filtration, centrifugation,

215 parative study of nanostructured PuO2 and Pu colloids produced by sonochemical and hydrolytic methods

216 The clay and zeolite colloids produced in these experiments are similar to th

217 Biogenic colloids, products of the manganese oxidase, Mnx, were s

218 The presence of colloids promotes the breakthrough of ciprofloxacin (ove

219 ing class of materials based on redox active colloids (RACs) that are inherently modular in their des

220 ative linkage is herein demonstrated for (i) colloids ranging from nano- to microscale; in two field-

221 eory, extended colloid filtration theory and colloid release model.

222 Fluorescent complex colloids represent a new approach for biosensing in liqu

223 a more stable association of plutonium with colloids, resulting in lower desorption rates.

224 eported to both increase as well as decrease colloid retention.

225 Characterization of Pu colloids revealed a correlation between the number of Pu

226 article-particle interactions of traditional colloid science are augmented by a family of nonequilibr

227 or which QCM can be exploited, especially in colloid science.

228 RS) using simple and widely available silver colloid SERS substrate.

229 Factors such as colloid size and the chemical composition of the OM may

230 Trends in retention as a function of colloid size were examined using nano- to microsized (0.

231 served contrasting retention and trends with colloid size.

232 roughness operates, attachment of a range of colloid sizes to glass with three levels of roughness wa

233 l orders of magnitude greater removal of all colloid sizes were observed in granular relative to thos

234 recisely controlling the 2D motion of active colloids so that their path has a nontrivial topology.

235 It is not known if use of colloid solutions containing hydroxyethyl starch (HES) t

236 zable transitions take place in concentrated colloids solutions.

237 or the highest storage modulus of the mixed colloids solutions.

238 MS confirmed the presence of various NPs and colloids, some containing aromatic compounds as well as

239 na including surface adhesion, friction, and colloid stability but their contribution on nanoparticle

240 UV) irradiation chamber was used to decrease colloid stabilization and metal-complexing capacity of N

241 face-active materials such as surfactants or colloids stabilize structures against coalescence and al

242 dynamics and the time-dependent response of colloids subject to a small external perturbation in a d

243 ssumption of depletion of the fast-attaching colloid subpopulation by attachment to grain surfaces pr

244 es in the synthesis and assembly of specific colloids such as the colloidal molecules as defined by v

245 Fe oxyhydroxide, Al(OH)(3), or clay mineral colloids, suggesting that the V is not bioavailable.

246 ining the mesoscopic order of liquid crystal colloids, suggesting that this feature may be a potentia

247 is dictated by molecular orientation at the colloid surface.

248 ultiple asperities acting within the zone of colloid-surface interaction were unable to produce the o

249 d spherical poly(methyl methacrylate) (PMMA) colloids, suspended in an apolar organic medium.

250 low cell desorption experiments with mineral colloid suspensions produced by hydrothermal alteration

251 Three different colloid suspensions were used: (1) colloidal material fr

252 ant to a variety of inclusions, ranging from colloids suspensions to multi-emulsion systems.

253 In this context, experiments based upon colloid synthesis and nanofabricated structures are assi

254 Silver colloids synthesized by reduction of AgNO3 by trisodium

255 CR initiator from a solid interface to AgNPs colloid system by toehold exchange-mediated strand displ

256 The stability variation of the colloid system can then be monitored by recording corres

257 aims at promoting the development of MOFs as colloids, taking ZIF-8 as a pioneering and successful ca

258 the enhanced self-assembly of triblock Janus colloids targeted to form a kagome lattice.

259 and the solvation of a large, highly charged colloid that exhibits overcharging, a complex nonlinear

260 perimental study directly tracks fluorescent colloids that are either stable in suspension or have at

261 rorheology on other systems of dense, jammed colloids that are highly scattering.

262 sembly in mixtures of chemically interacting colloids that are known to exhibit nonreciprocal effecti

263 Active colloids, that consume energy to move, hold similar pote

264 drupolar(8-12) and hexadecapolar(13) nematic colloids, the symmetries of such elastic distortions mim

265 Inspired by patchy colloid theory, we propose a general framework by which

266 lized as heteroaggregates with the kaolinite colloids they were attached to when favorable conditions

267 known about the dynamic transformation from colloid to superlattice.

268 Coulombic self-assembly enables conventional colloids to be used as model colloidal ions, primed for

269 ntly attribute the IRI of AF(G)P-inspired Au colloids to the Kelvin effect.

270 Reactivity of the synthetic colloids toward reduction by Mn(2+), in the presence of

271 cale interactions via mechanistic pore-scale colloid trajectory simulations that predicted and define

272 detectable microbial tracers for subsurface colloid transport and water flow.

273 f diffusiophoresis as a means to control the colloid transport in dead-end channels by introducing a

274 ulation balance modelling approach and other colloid transport theories, have been incorporated into

275 r emulsions and macro hydrogels that are gel colloid type.

276 mic flow field around a catalytically active colloid using particle tracking velocimetry both in the

277 proportion of U associated with the 1-3 kDa colloids varied spatially and seasonally.

278 brated to experimentally observed tangential colloid velocities, demonstrating that slip length was e

279 te for smaller (<200 nm) and larger (>2 mum) colloids was observed and discussed.

280 The chemical fingerprint of the colloids was obtained by pyrolysis coupled with gas chro

281 The band-gap energies of the colloids were found to increase with decreasing hydrodyn

282 Synthetic colloids were prepared by thiosulfate reduction of perma

283 egrees C colloids and the Pu-montmorillonite colloids were similar while the desorption rates from th

284 The colloids were studied optically and via NMR as they aged

285 the desorption rates from the 200 degrees C colloids were up to an order of magnitude lower.

286 For comparison, similar charged colloids were used to create an interface between a face

287 ent in the form of organic and organomineral colloids, which also account for the majority of dissolv

288 oding unconventional assembly in anisometric colloids, which can likely introduce properties and phas

289 ng yet underexplored third type: anisometric colloids, which integrate micrometer and nanometer dimen

290 ionic strength were ineffective at releasing colloids while in the presence of Th(IV), decreases in i

291 tions due to a lack of means to produce such colloids with a well-controlled variable Janus balance.

292 diagrams open a pathway to a large family of colloids with complex architectures and unusual chiropti

293 high-order elastic multipoles emerging when colloids with controlled shapes and surface alignment ar

294 mbly of both proteinaceous shells and patchy colloids with dissociable charge groups.

295 Here, we show that spherical colloids with metal patches of low symmetry self-propel

296 Janus colloids with one attractive patch on an otherwise repul

297 Porous carbon spheres derived from polymer colloids with regular geometry, monodispersed morphology

298 Here we develop nematic colloids with strong elastic monopole moments and with e

299 attached onto the surface of well-defined Au colloids with the same sizes but different shapes.

300 xplore experimentally random packings of dry colloids with X-ray nanotomography that directly provide