ライフサイエンスコーパス: particle

1 d pharmacophores (or from drug loaded porous particles).

2 anded DNA (polymer) and condensing proteins (particles).

3 distance between the fiber tips and trapped particle.

4 replication and the generation of infectious particles.

5 gh a bed packed with millimeter-size calcite particles.

6 of closely associated or physically similar particles.

7 sometry is sensitive to geometric changes of particles.

8 ease of 18S-E from Bystin-associated pre-40S particles.

9 ms, which subsequently ingest the stabilized particles.

10 rnating between clustering and dispersion of particles.

11 distinguishes active particles from Brownian particles.

12 ly among binding locations, inside rotavirus particles.

13 0.03 +/- 0.009 with aqueous glycine aerosol particles.

14 n the plasma pool sizes of these lipoprotein particles.

15 lipid composition of producer cells and HIV particles.

16 ors PA28alphabeta and PA28gamma bound to 20S particles.

17 -(thiotriphosphate) (ATPgammaS) than with WT particles.

18 tion was mainly from accumulation and coarse particles.

19 oth resulted in nucleation and growth of SOA particles.

20 the fermentation supernatant using magnetic particles.

21 irus assembly and in the morphology of virus particles.

22 ucture during the self-assembly of CCMV-like particles.

23 owed by CaCl2 addition resulting in hardened particles.

24 in budding or being incorporated into virus particles.

25 range of 0-Dimensional (0D) objects such as particles, 1D nanowires and fibres, 2D films and coated

26 ng efficiency was 20 to 50%; of the uncoated particles, about 10 to 15% synthesized detectable RNA.

27 Here, we introduce a class of particle absorbers called transferable hyperbolic metama

28 ents can certainly be made that linear-field particle acceleration in free space is very doubtful giv

29 Brownian dynamics simulations for different particle actuation configurations.

30 pture rates are enhanced by applying dynamic particle actuation, resulting in an increase in the asso

31 tion of a fast gas-sampling valve and a soot particle aerosol mass spectrometer (SP-AMS) enabled onli

32 We reasoned that small particle aerosols of virus would penetrate the lower res

33 size reduction to 20 nm leads to significant particle agglomeration, thus decreasing the activity.

34 compatibility and circumvents the problem of particle agglomeration.

35 bed to an accretion disk corona of energetic particles akin to those seen in the solar corona.

36 s data acquisition method for cryo-EM single-particle analysis with the Volta phase plate.

37 The method uses solute gradients to induce particle and fluid motions via diffusiophoresis and diff

38 could be responsible for the elicitation of particle and ion release and whether these released impl

39 both sensitive to the zeta potential of the particle and the wall.

40 ct originally introduced to model elementary particles and a baby skyrmion is its two-dimensional cou

41 e the NHC being coordinated to the palladium particles and affecting their electronic properties.

42 sing their strength such as doping with fine particles and alloying often significantly decrease thei

43 Phagosomes form during engulfment of large particles and become increasingly acidic and proteolytic

44 on is lowest for the more highly coordinated particles and decreases during sintering.

45 stigated the planktonic MGII associated with particles and in free-living forms in the Pearl River Es

46 spreading centers, both in the form of plume particles and seafloor massive sulfide structures.

47 )) indicated strong interactions between nCu particles and SRE, as well as with individual organic ac

48 .3-MDa prokaryotic 30S, 50S and 70S ribosome particles and the 9-MDa Flock House virus.

49 ted to be by both the direct action on virus particles and the interference on the host cells.

50 n between the aspect ratio r of the absorbed particles and the slope and intercept of the line that f

51 been confounded by defective, noninfectious particles and the stochastic minefield blocking access t

52 s-gold nanoparticles appear mostly as single particles and they cluster during the vesicular transpor

53 can be used to trace the sources of ambient particles and to know their potential impacts in human h

54 ous and branched respiratory syncytial virus particles, and assembly with genomic ribonucleoproteins

55 rporates more VP26 fusion protein into virus particles, and individual virus particles exhibit bright

56 accumulation of hemolymph proteins, dextran particles, and silver nitrate.

57 ws for rapid and robust synthesis of complex particles, and the latter can be used to assemble such p

58 n for medium and large number of interactive particles, and uses tools and concepts from density func

59 hat these are formed in the tissue as 400-nm particles; and that they attach to the surface of coral

60 Interestingly, single particles appear to exhibit target depletion zones near

61 nt changes in the size and morphology of the particles; approximately 15 nm aggregates consisting of

62 Further, since single particles are detected unbound in flow, the technique ca

63 Once the Sn+1 particles are formed, they may further nucleate to form

64 The particles are fully degradable in response to esterases

65 In contrast to the synthetic systems, LDL particles are intrinsically biocompatible and biodegrada

66 t virus, suggesting that a fraction of virus particles are resistant to antibody neutralization despi

67 lycoproteins (Envs) on the surfaces of HIV-1 particles are targeted by host antibodies.

68 These particles are then stabilized through ultraviolet irradi

69 Nano-sized Pd particles are uniformly dispersed on graphene nanosheets

70 These novel quasi-particles arguably explain a range of poorly understood

71 ocessing was developed to count and sort the particles as a function of their size and thus determine

72 which enabled us to image single fluorescent particles as small as 50 nm in diameter and single quant

73 One-dimensional conductive particle assembly holds promise for a variety of practic

74 other in some, but not all, aspects of virus particle assembly.

75 Our results suggest that these particle-associated and free-living bacterial assemblage

76 pally as small (<0.45 mum) iron oxyhydroxide particles at pH 8 with only approximately 3-27% present

77 confocal microscopy, we observe the initial particle attachment to the membrane, then particle wrapp

78 ructured illumination microscopy with single-particle averaging to localize 14 S. pombe SPB component

79 The dual mineralized particle-based system can specifically release Ex4 while

80 come relevant for suspensions of microscopic particles, behaving as "billiard balls" in a liquid, in

81 end on conformation, with regular, spherical particles being delivered to a greater extent than long-

82 5 (PM = particulate matter), PM10, ultrafine particles, black carbon, and the elemental composition o

83 r the Snake River particles, indicating that particle-bound, or sorbed Zn, was bioavailable from acid

84 are extremely bright, photostable, nanometer particles broadly used to investigate single molecule dy

85 y increasing the efficiency with which virus particles bud from infected cells and restoring filament

86 while having limited effects on total virus particle budding.

87 endent on the cluster morphology and size of particles but the origin of this dependence is largely d

88 cytic uptake of bacterial (Escherichia coli) particles by (i) capturing along the filopodial shaft an

89 ted water consists of dissolution of calcite particles by flow of acidified desalinated water through

90 us, RNA synthesis by even a single, uncoated particle can initiate infection in a cell.IMPORTANCE The

91 these acid-degradable cationic nanohydrogel particles can be considered as promising siRNA carriers

92 Moreover, integration of mineralized particles can enhance the mechanical strength of alginat

93 Asymmetric particles can exhibit unique properties.

94 olenses are rapidly formed around each virus particle captured on the substrate using a portable inte

95 lementary existing fields indicate potential particle, chemical and microbial hazards.

96 apped energetic protons, electrons and other particles circulate at altitudes from about 500 to 40,00

97 A strategy to halt dissolution of particle-coated air bubbles in water based on interfacia

98 mixed with increasing amounts of metal-rich particles collected from two acid mine drainage impacted

99 eters (SPMSs), which generate in situ single particle composition data, are excellent tools for chara

100 Organic carbon in atmospheric particles comprises a large fraction of chromatographica

101 th collision frequency (beta) and background particle concentration (B) to be independent for use in

102 PM2.5 and carbonaceous particle concentrations have been declining appreciably

103 alls as a function of species volatility and particle condensational sink.

104 res of a polymer and nonspecifically binding particles (condensers) are studied as models for viruses

105 using lectin microarrays and lectin-magnetic particle conjugate-assisted LC-MS/MS analyses.

106 m full to partial depletion, with 24% of SSA particles containing chloride (mole fraction of Cl/Na >/

107 Here we show that inactivated rabies virus particles containing the MERS-CoV S1 protein induce pote

108 lead to a significant increase in the total particle counts due to the formation of self-nucleated m

109 n 6S RNA and Esigma(70) determined by single-particle cryo-electron microscopy and validation of the

110 he effects of specimen orientation in single particle cryo-EM and present open-source software for ra

111 d propeller forms, were determined by single-particle cryo-EM at 3.9 A and 5.6 A, respectively.

112 Here, we describe a 3.6 A single-particle cryo-EM reconstruction of the core CBF3 complex

113 the authors present the CVA6 procapsid and A-particle cryo-EM structures and identify an immune-domin

114 The favorable properties of hydrogel particles depend largely on their size, and particles ra

115 rmation of colloidal capsules, the colloidal particle deposition on (sacrificial) templates, the amph

116 between neighboring redox units of clustered particles (Dh,DLS = 195 nm) and the mono- and trinuclear

117 In contrast, particle diffusometry permits in situ analysis of DNA mi

118 Examining the ensemble of particle displacements reveals a Laplace distribution at

119 a transcriptionally competent, double-layer particle (DLP), which they deliver into the cytosol.

120 remain strictly positive only when the fast particle dynamics reveal two or more ergodic components

121 With recent advances in single-particle electron cryo-microscopy (cryo-EM) data process

122 ure of Drosophila NOMPC determined by single-particle electron cryo-microscopy.

123 nalyses of antigen-antibody complexes.Single-particle electron cryomicroscopy (cryoEM) can circumvent

124 Intratracheally administered sildenafil particles elicited more pulmonary specific and sustained

125 Furthermore, single-particle EM analysis revealed, for the first time, the o

126 FeNx Cy moieties are more selective than Fe particles encapsulated in N-doped carbon.

127 computationally predict the impact of local particles' environment on the recorded IR spectra.

128 er mass (toxicity) was highest for ultrafine particles, estimated lung deposition was mainly from acc

129 n into virus particles, and individual virus particles exhibit brighter red fluorescence.

130 This model was extended to charged particle exposures by integrating Monte Carlo calculated

131 iably since 2010/11 due to the use of diesel particle filters, but little change is seen in nitrogen

132 collision and oxidation is imaged by single-particle fluorescence microscopy.

133 omponents, including the line-focused laser, particle focusing using multinode acoustic standing wave

134 These proteins prime the particle for removal by immune cells and may contribute

135 Utilizing colloidal particles for the assembly of the shell of nano- and mic

136 sive laser probes should give insight on the particle formation mechanisms and may lead to better-con

137 The exudate has a stabilizing effect on the particles formed with decreased aggregation rate and inc

138 a crucial property that distinguishes active particles from Brownian particles.

139 important to document properties of primary particles from combustion sources, which can be used to

140 dal sediment size, by tracking the motion of particles from the surface to deep inside the bed, and f

141 free radicals, thereby strongly influencing particle growth rate and the resulting particle morpholo

142 e course is characteristic of nucleation and particle growth; rates for these processes followed expe

143 The larger particles (>5 mum in diameter) of bioaerosol settle and

144 id) of capsid-RNA interactions, the two CVA6 particles have essentially identical atomic capsid struc

145 Importantly, these FV(+) particles have the same size distribution as infused hum

146 Maxwell's equations, suggest that colloidal particles heated or cooled in certain polar or paramagne

147 Paramagnetic particles heavily decorated with anti-ERalpha antibody a

148 Successfully assembled cell-particle hybrids presented here comprised either melanom

149 ed Plasma Mass Spectrometry (ICP-MS), single-particle-ICP-MS (sp-ICP-MS), Transmission Electron Micro

150 free method for the automatic recognition of particle images from cryo-EM micrographs.

151 he composition and organization of the viral particle.IMPORTANCE Tailless viruses of the family Tecti

152 al fusion, for fabricating functional patchy particles in a tunable and scalable manner.

153 licited by immunization via Pfs25 virus-like particles in human immunoglobulin loci transgenic mice.

154 used for apportioning sources of atmospheric particles in late fall in Innsbruck.

155 s virus (PRV) and herpes simplex virus (HSV) particles in living cells.

156 aggregation rates (alphabetaB) to background particles in mixed systems is also experimentally valida

157 its a Cdc48 hexamer to extract them from 60S particles in order to escort them to the proteasome for

158 d that estimate the relative surface area of particles in the detector, taking into account the effec

159 cost linearly proportional to the number of particles in the system.

160 ins, and the suppression of big second phase particles in this 3.2 mum thick REBa2Cu3Ox film.

161 A thorough physical characterisation of the particles included transmission electron microscopy, X-r

162 escently labeled ligands and small diffusing particles, including nanodiscs and liposomes containing

163 optimised in order to increase the volume of particle incorporation.

164 s River particles to 45% for the Snake River particles, indicating that particle-bound, or sorbed Zn,

165 hin residues 44-65 against reconstituted HDL particles, indicating that these mAbs specifically recog

166 Thus, ultrafine particles ingestion alters gut microbiota composition, a

167 laying the role of the fundamental number-of-particles integral of motion of the nonlinear Schrodinge

168 CD14(+) cells were overall more efficient at particle internalization compared with the four other po

169 and the latter can be used to assemble such particles into bulk materials.

170 ating photoacoustic responses that can drive particles into the medium, guided by magnetomotive force

171 on, where interference appears even when the particle is localized.

172 Ice formation on aerosol particles is a process of crucial importance to Earth's

173 to which depletion processes deplete non-EV particles is incompletely understood, but depleted serum

174 h [Formula: see text] 1 [Formula: see text]m particles is presented and discussed.

175 The size of catalyst particles is tunable through synthesizing Fe-doped ZIF n

176 from pre-formed RNPs deposited by infecting particles is unaffected.

177 Recently, Ballottari et al., analyzing PSI particles isolated from an Arabidopsis thaliana mutant t

178 elemental characteristics of leaf deposited particles, joined with the leaf magnetic content, may su

179 Here, we extracted MP-like particles larger than 149 mum from 17 salt brands origin

180 e most frequently observed in individual LSA particles less than 0.5 mum in diameter.

181 Single particle mass spectrometers (SPMSs), which generate in s

182 165I) restored polyprotein processing, virus particle maturation, and significant levels of replicati

183 lly different and that the interplay between particle microhabitats and surrounding geochemical regim

184 riving (i.e., 3.34 x 10(12) to 2.29 x 10(13) particles/mile) were larger than those measured on urban

185 routes (i.e., 5.06 x 10(11) to 1.31 x 10(13) particles/mile).

186 more) residential black carbon +5.33 x 10(5) particles/ml higher carbon load (95% confidence interval

187 dence interval, 1.56 x 10(5) to 9.10 x 10(5) particles/ml) for an interquartile range increment in an

188 average (SD) of 98.2 x 10(5) (29.8 x 10(5)) particles/ml.

189 We demonstrate that particle morphology and evaporation is dependent on whet

190 ct contributions to Gag-Gag oligomerization, particle morphology, and biogenesis.

191 ncing particle growth rate and the resulting particle morphology.

192 mammalian cells affects the dynamics of IFT particle movement.

193 Particle number (PN) emissions were 28% and 17% higher w

194 By measuring the particle size and the particle number distribution, we were able to calculate

195 ted Ddx4, [Formula: see text], diffuses as a particle of 600-nm hydrodynamic radius dissolved in wate

196 based on affinity binding with ferromagnetic particles of azocasein composite (mAzo).

197 releasing resins containing micrometer-sized particles of Bioglass 45S5 (BAG) or fluoride-containing

198 pulses in aqueous monolayers of micron-sized particles of controlled microstructure.

199 mainly in the perpendicular direction, while particles of less than 30mum remained suspended and trav

200 Wheat flour particles of more than 60mum (released in air by sifting

201 Thus, we prepared porous PLGA particles of sildenafil using a water-in-oil-in-water do

202 and morphological dynamics of a single, same particle on nanometer and ultrashort time scales.

203 mechanism results in a higher attachment of particles on oil in comparison with adsorption, as commo

204 The effects of the fine particles on the UHI reduction were limited to the lowes

205 f the silver island exceeds that of the gold particles, only quasi-occupation of the silver transfer

206 Despite the presence (in A-particle) or absence (in procapsid) of capsid-RNA intera

207 ral HDL quality-related characteristics (HDL particle oxidation, resistance against oxidative modific

208 We consider an active particle performing a blind cruise search for nonregener

209 quantify these effects, we measured gas- and particle-phase emissions from 82 light-duty gasoline veh

210 e area (r(2) approximately 0.5-0.7), rate of particle-phase reaction (r(2) approximately 0.4-0.7), an

211 n the two signals to create a mapping of the particle position to resistive pulse amplitude at the sa

212 xhibit pixel locking, in which the estimated particle positions concentrate toward the centers of pix

213 The synthesized particles possess potential characteristics for targeted

214 , we focus on a imidazolium based IL and use particle-probe rheology to (i) catch this phenomenon and

215 Detection limit for the particles produced by the laser ablation of a copper foi

216 ctin cytoskeleton severely reduced net virus particle production.

217 tending the lifespan of virus reservoirs and particle production.

218 iral RNA are required for the enhancement of particle production.

219 mic-like substances (HULIS), which influence particle properties and impact climate, human health, an

220 oblem of extracting information on intrinsic particle properties from the whole class of interacting

221 ished theories, such nonuniformly magnetized particles provide greater magnetic stability than their

222 a is the viscous penetration depth, a is the particle radius, Deltaf is the QCM frequency shift, and

223 Chloride content of SSA particles ranged from full to partial depletion, with 24

224 particles depend largely on their size, and particles ranging from nanometers to micrometers are use

225 phosphorus concentrations, control elemental particle ratios.

226 its, crystalline solids flow plastically via particle rearrangements localized around structural defe

227 ion and mRNA cargos of the ribonucleoprotein particles (RNPs) that form the substrate for axonal tran

228 We find that the rate of particle rotation is lowest for the more highly coordina

229 g the range of the repulsive force below the particle roughness suppresses the frictionless state and

230 due to an embedded ester cross-linker in the particle's core.

231 to an interplay between time-dependent many-particle scattering and phase-space filling effects.

232 rate robust fiber formation for a variety of particle shapes and aggregation conditions.

233 lation of GEOs in water-based microemulsion (particle size 10.1nm) showed better antimicrobial activi

234 in consumer products, there is evidence that particle size and formulation influences skin permeabili

235 ze and shape spectrum' (SSS) includes litter particle size and shape and their consequent effect on f

236 We describe the effect of varying particle size and shape on the SERS signal, focusing on

237 By measuring the particle size and the particle number distribution, we w

238 ) concentration, relative humidity (RH), and particle size control reaction rates and mechanisms.

239 We measured particle size distribution of wheat flour, photographed

240 unction of their size and thus determine the particle size distribution.

241 racer exchange data sets that explore pH and particle size effects, we developed a stochastic simulat

242 Particle size was controlled by the concentration of the

243 True density increased with decreased particle size whereas porosity and bulk density increase

244 atic effects on important properties such as particle size, charge, and solubility.

245 l, and cobalt) were synthesized with average particle sizes from 0.9 to 1.4 nanometers, with tight si

246 The developed nanocarriers presented particle sizes ranging from 71 to 366nm, leading to exce

247 uences skin permeability and that lipophilic particles smaller than 6 nm can embed in lipid bilayers.

248 nd bone formation was highly impacted by the particle-specific agglomeration behaviour in this study.

249 e dominated (73-83%) by the intrinsic single particle spectral broadening, as observed using spectral

250 CGMMV's particle stability, ease of contact transmission, and se

251 The HTLV-1 particle structure is still poorly understood, and previ

252 evelopment programs, knowledge of flavivirus particle structure, definition of E dimers as the key an

253 cumulated 18S-E in Bystin-associated pre-40S particles, suggesting that the enzymatic activity of PAR

254 re conducted to study the correlation of the particles' surface charge density with their translocati

255 as a function of size or chemically distinct particle surfaces can determine the hygroscopicity of pl

256 The paper presents a novel two-stage particle swarm optimization (PSO) for the maximum power

257 the whole class of interacting magnetic fine particle systems is a long standing and difficult invers

258 ttle is known about the in vivo fate of drug particles taken orally, in particular, the drug release

259 a poorly understood form of the dimeric 70S particle that has been linked to pathogenesis, translati

260 irus genomes relative to the number of viral particles that can form plaques in culture is much lower

261 omagnetic field fluctuations and the charged particles that comprise an undamped kinetic Alfven wave.

262 of described nanoparticles suggest that the particles that do not induce pro-inflammatory cytokines

263 ficient cell culture system and isolated HEV particles that were infectious in vitro and in vivo.

264 y by coating their surface and binding phage particles, thereby preventing their attachment to the ce

265 The particles therefore represent a suitable base material t

266 called transferable hyperbolic metamaterial particles (THMMP) that display selective, omnidirectiona

267 ffinity of nanoparticles obtained by flowing particles through a porous medium are constrained by the

268 s before they are translocated into the core particle to be degraded.

269 cy (AE) varied from 28% for the Animas River particles to 45% for the Snake River particles, indicati

270 that gE/gI and US9 function by tethering HSV particles to kinesin microtubule motors.

271 d feedstream impurities cause these catalyst particles to permanently deactivate.

272 uch higher (4,000- to 20,000-fold increased) particle-to-PFU ratio in vitro than herpes simplex virus

273 However, in the limit of vanishing particle-to-wall mass ratio, the equilibration rates rem

274 les coupled to the DNA strands that link the particles together, in the form of a rhombic dodecahedro

275 Using a 3D particle tracking method, the authors show that the smoo

276 Mechanistically, single-particle tracking revealed that E2 treatment selectively

277 he mobile lo domains by video microscopy and particle tracking showed that the domains' mobility is s

278 ing recently developed live cell imaging and particle-tracking methods for studying bacterial-endothe

279 fficient of SO2 (gammaSO4(2-),light) for GDD particles under UV light compared to the value (gammaSO4

280 Within the endosome, particles undergo a series of stepwise disassembly event

281 e outer and inner (pore) surfaces of biochar particles using high-resolution spectro(micro)scopy and

282 rned with Toll-like receptor-9 ligand-loaded particles using streptavidin-biotin cross-linking.

283 s modeled by multiple millions of mesoscopic particles-using a single shared memory commodity worksta

284 ivalent GI.1 and GII.4c norovirus virus-like particle (VLP) vaccine candidate adjuvanted with alum an

285 nding strength of Zn sorption to the natural particles was inversely related to Zn bioavailability; a

286 Using a minimal model of ill-fitting, sticky particles, we demonstrate robust fiber formation for a v

287 The particles were characterized for their optical propertie

288 Particles were tracked simultaneously in the two signals

289 (MSA) reacts with amines and ammonia to form particles, which is expected to be particularly importan

290 The space-spanning immobile particles, whose population is sensitive to the cooling

291 sing through both slits, we have a localized particle with nonlocal interactions with the other slit.

292 00 nm spatial resolution for phase separated particles with a approximately 150 nm shell and 300 nm c

293 onstrate self-assembly to nanoscale cuboidal particles with a bicontinuous cubic structure by amphiph

294 uidized bed CO2 capture systems due to large particles with a diameter up to 1200 mum and irregular o

295 NOM) alone due to formation of smaller CaCO3 particles with a much more negative zeta-potential.

296 mponent mesoporous carbon-organosilica Janus particles with asymmetric wettability are synthesized th

297 icron SSA tend to be spatially heterogeneous particles with sodium- and chloride-rich cores surrounde

298 to carry therapeutic oligonucleotides, while particles with strong interferon and mild pro-inflammato

299 al particle attachment to the membrane, then particle wrapping, and in rare cases spontaneous membran

300 s for substrate deposited individual sucrose particles, Young's modulus and surface tension can be qu