ライフサイエンスコーパス: air-water interface

1 ge bonded and transported the arsenic to the air-water interface.

2 gh physicochemical processes at and near the air-water interface.

3 tides leads to enriched fibrillization at an air-water interface.

4 urface of water, and quickly dive across the air-water interface.

5 e reactivity of Criegee intermediates at the air-water interface.

6 had the largest force due to pinning of the air-water interface.

7 ugh an unusual monolayer intermediate at the air-water interface.

8 loosely packed or arrested structures on the air-water interface.

9 sembly of beta-sheet-forming peptides at the air-water interface.

10 its ability to form continuous layers at the air-water interface.

11 nd the two-dimensional melting in MLF at the air-water interface.

12 s consistent with its role in stabilizing an air-water interface.

13 nd orientation alignment of nanowires at the air-water interface.

14 ecome surface active and are enriched at the air-water interface.

15 favorable exposure of H atoms of H2O at the air-water interface.

16 nolayer containing the receptor GM(1) at the air-water interface.

17 y oriented within Langmuir monolayers at the air-water interface.

18 ent of the QDs in the monolayer films at the air-water interface.

19 ineer the 2D self-assembly of the QDs at the air-water interface.

20 fluorescence microscopy of monolayers at the air-water interface.

21 "reservoirs" of fluid phase adjacent to the air-water interface.

22 a dense band at a certain distance from the air-water interface.

23 rm of dSP-C is not surface-associated at the air-water interface.

24 l iron-nickel cyanide-bridged network at the air-water interface.

25 and SP-C in lipid-protein monolayers at the air-water interface.

26 triple-stranded beta-sheet monolayer at the air-water interface.

27 ble into two-dimensional crystallites at the air-water interface.

28 haracteristic of an edge-on structure at the air-water interface.

29 emplating method (template-inhibition) at an air-water interface.

30 from the appropriate monolayer phase at the air-water interface.

31 spholipid monolayers was investigated at the air-water interface.

32 it adsorption of pulmonary surfactant to the air-water interface.

33 digestion, both in bulk and adsorbed at the air-water interface.

34 neous monolayers at constant pressure at the air-water interface.

35 e when spread on top of a urease film at the air-water interface.

36 is either nonexistent or inaccessible at an air-water interface.

37 layer of monodendrons during collapse at the air-water interface.

38 = CH3; and for CH3NH2, R1 = R2 = CH3) at the air-water interface.

39 an iminodiacetate-Cu(II) lipid spread at the air-water interface.

40 e of domain sizes in lipid monolayers at the air-water interface.

41 that can spread rapidly from solution to the air-water interface.

42 ine both increase the surface tension at the air-water interface.

43 reaction mechanism of singlet oxygen at the air-water interface.

44 rated compounds by chemical reactions at the air-water interface.

45 id proxy which formed an organic film at the air-water interface.

46 isopropyl methyl groups of l-leucine at the air-water interface.

47 perties of pulmonary surfactant films at the air-water interface.

48 ical force to its molecular monolayer at the air-water interface.

49 ic behavior of syn- and anti-CH3 CHOO at the air-water interface.

50 ot even capable of forming monolayers at the air-water interface.

51 muir films was systematically studied at the air-water interface.

52 of a sequence-specific peptoid polymer at an air-water interface.

53 h and polycrystalline circular assemblies on air-water interface.

54 ne photolysis by UV and visible light at the air-water interface.

55 yers containing Gb3 were investigated at the air-water interface.

56 ion selectively forming peptide bonds at the air-water interface.

57 parated from the solution and floated at the air/water interface.

58 ctivity of volatile organic compounds at the air/water interface.

59 Additional studies were performed at the air/water interface.

60 pid adsorption of pulmonary surfactant to an air/water interface.

61 to the parallel beta-sheet structure at the air/water interface.

62 anced concentrations of selected ions at the air/water interface.

63 the value determined for thiocyanate at the air/water interface.

64 rbles" that remain stable when placed at the air/water interface.

65 itially lie flat on the water surface at the air/water interface.

66 electrolyte ions between bulk water and the air/water interface.

67 metry with line microelectrodes touching the air/water interface.

68 ant entropy contribution, in contrast to the air/water interface.

69 esidue beta-hairpin peptides adsorbed at the air/water interface.

70 ually exhibit enhanced concentrations at the air/water interface.

71 ectron hopping in Langmuir monolayers at the air/water interface.

72 onal order in monolayer films in situ at the air/water interface.

73 d peptide secondary structure in situ at the air/water interface.

74 ives with SDS for available positions at the air/water interface.

75 opropylacrylamide) (PNiPAm) microgels at the air/water interface.

76 e reported out-of-plane reorientation at the air/water interface.

77 central triptycene core are confined at the air/water interface.

78 ntus, a singly flagellated bacterium, at the air/water interface.

79 he adsorption of the surfactant lipids to an air/water interface.

80 es start and run autonomously when placed at air-water interfaces.

81 ete Pythium ultimum that was grown along the air-water interfaces.

82 corporation of lipids into monolayers at the air-water interface after collapse is important to the m

83 anges in the amide I spectra of hIAPP at the air/water interface after addition of dipalmitoylphospho

84 artitioning of hydrophobic proteins into the air-water interface and allows imaging of the foam struc

85 tructural changes to lipid monolayers at the air-water interface and bilayers at the solid-water inte

86 n and at hydrophobic-hydrophilic interfaces (air-water interface and phospholipids).

87 the nanodrops is similar to that at the bulk air-water interface and that the hydrogen bonding of int

88 to quantify the capillary forces between an air-water interface and the different particles.

89 ionization state of organic molecules at the air-water interface and the related problem of the surfa

90 e suspensions could then be dispersed at the air-water interface and transferred to silicon wafers us

91 ynthesis of a two-dimensional polymer at the air/water interface and its nm-resolution imaging.

92 ribes a two-dimensional polymerization at an air/water interface and provides, for the first time, di

93 s showed that EPL1 readily self-assembles at air/water interfaces and forms protein layers that can b

94 rties of BUBR1(1-204) and TPR-PP5(16-181) at air/water interfaces and found that both proteins exhibi

95 d a highly emissive face-on structure at the air-water interface, and did not form pi-aggregates.

96 udies of the behavior of the polymers at the air-water interface, and of the photophysical properties

97 ides were reconstituted as monolayers at the air-water interface, and their properties, as well as th

98 low foaming, high areas of occupancy at the air/water interface, and weak solid-adsorption and solub

99 uct are explainable only if reactions at the air-water interface are dominant.

100 dihydrocholesterol and phospholipids at the air-water interface are used to model membranes containi

101 A-induced ion pair particle formation at the air-water interface are yet to be examined.

102 ement of particles, depending on whether the air-water interfaces are stationary or mobile.

103 mitoylphosphatidylglycerol monolayers at the air/water interface are presented.

104 We use the hydrophobic environment of the air-water interface as a favorable venue for peptide bon

105 ze spherical and ellipsoidal particles at an air-water interface as a function of surface coverage.

106 CPA oxidation by OH in the gas-phase, at the air-water interface as well as in the solid phase (dry f

107 the field of 2D polymers synthesized at the air/water interface as it, in principle, allows estimati

108 ree-energy profile for a solute crossing the air-water interface, as well as the thermodynamic cost o

109 s the surface activity of the protein at the air:water interface, as determined by surface tension me

110 Here, we also report that on air-water interface, association of fullerene to pure an

111 ynthetic D-erythro C18-ceramide films at the air-water interface at various surface pressures (pi).

112 of xylem sap plays a key role in stabilizing air-water interfaces at the pits between water- and gas-

113 ine-(leucine)4]4-lysine (KL4), spread at the air/water interface at 25 degrees C and pH 7.2, and its

114 NP BTCs and indicated that attachment to the air-water interface (AWI) occurring during FI was the ke

115 In this work the effect of the air-water interface (AWI) on alpha-Syn aggregation is in

116 mer formation to be higher and faster at the air-water interface (AWI) than in the bulk (by 14 and ap

117 bibition efficiently released cells from the air-water interface (AWI) that were initially retained u

118 ns are repelled from water/hydrophobe (e.g., air/water) interfaces, both computer simulations and exp

119 These polymers were characterized at the air-water interface by Langmuir techniques and found to

120 Such interactions were studied at the air-water interface by Langmuir-Blodgett assembly.

121 hus, after the ellipsoids are carried to the air-water interface by the same outward flow that causes

122 nd transport, as particles can attach to the air-water interfaces by action of capillary forces.

123 methods was attributed to saturation of the air/water interface by a DTAB/trianion complex far below

124 pid adsorption of pulmonary surfactant to an air/water interface by an unknown mechanism.

125 erse polystyrene (PS) particle monolayers at air/water interfaces by using our needle tip flow method

126 ., viruses and proteins), the velocity on an air-water interface can be as large as approximately 47

127 roscopy of phase-separated monolayers at the air-water interface can be generated by the selective ad

128 These moving air-water interfaces can mobilize colloids.

129 mixed with cholesterol in a monolayer at an air-water interface, coexisting 2-dimensional liquid pha

130 protein and lipid-protein monolayers at the air-water interface confirmed that the residual dSP-C he

131 Bubbles that reached the outer air-water interface contained no (1)O(2).

132 the non-equilibrium crystalline phase on the air-water interface could be explained with a model that

133 illary force and the snap-off force when the air-water interface detaches from the particle.

134 visualized colloids interacting with moving air-water interfaces during capillary fringe fluctuation

135 lt, the Au wavy nanowires were driven to the air/water interface during the synthesis.

136 whey and acid bovine whey were preserved at air water interface even after a heat treatment at 90 de

137 tering that nanoparticle membranes formed at air/water interfaces exhibit a small but significant app

138 thyl-1-piperidynyloxy radical (Tempo) to the air/water interface follows a Langmuir isotherm.

139 e transition temperatures and behavior at an air-water interface for this series are similar to phosp

140 -(N-isopropylacrylamide) was adsorbed at the air/water interface for this purpose.

141 the bordered pit chamber such that a convex air-water interface forms at the entrance into the pit c

142 Biosurfactants at the air-water interface generated by microorganisms as a res

143 likely create a small negative charge at the air-water interface, generating an electric double layer

144 The air-water interface has also attracted much interest as

145 eramide (GM(1)), in a lipid monolayer at the air-water interface has been studied utilizing grazing i

146 Solid surfaces and air-water interfaces have been shown previously to promo

147 Monolayers at the air/water interface have received considerable attention

148 Molecular areas of soluble films at the air/water interface have traditionally been calculated b

149 The results show that, at the air-water interface, HMSA deprotonates within a few pico

150 The apparent simplicity of the air/water interface, however, masks an underlying comple

151 (i) they self assemble into monolayers at an air/water interface; (ii) the monolayers are dominated b

152 zeolite nanosheet monolayer is formed at the air-water interface in a conical Teflon trough.

153 e to photochemical reactions occurring at an air-water interface in presence of model saturated long

154 s study, the micron-scale Haines jump of the air-water interface in rough fractures was investigated

155 c-hydrophilic interfaces, represented by the air-water interface in vitro and diverse heterogeneous i

156 g self-assembly of protein aggregates at the air-water interface in which initial foam formation is f

157 ed by hydrophobic-hydrophilic interfaces (an air-water interface in-vitro or membranes in-vivo).

158 loped a laboratory model microcosm mimicking air-water interfaces in soil.

159 hanging water tables lead to displacement of air-water interfaces in soils and sediments.

160 y glass bead surface were detached by moving air-water interfaces in the capillary fringe.

161 chemicals to calibrate mass transfer at the air/water interface in a fugacity-based multimedia model

162 film that lowers the surface tension of the air/water interface in the lungs.

163 tant, a lipid/protein complex that lines the air/water interface in the mammalian lung, functions to

164 Chemistry at the air/water interface, in particular, is still poorly unde

165 re we measure the surface deformation at the air-water interface induced by continuous and pulsed las

166 ing about how these reactions proceed at the air-water interface is needed.

167 The air-water interface is perhaps the most common liquid in

168 system is spatially non homogeneous (i.e. an air-water interface is present).

169 Exploration of their behavior at the air-water interface is reported and analyzed in terms of

170 Lung surfactant adsorption to an air-water interface is strongly inhibited by an energy b

171 The molecular characterization of the air/water interface is a key step in understanding funda

172 s for the study of monolayers in situ at the air/water interface is evident from this work.

173 compressional instability of particle-laden air/water interfaces is investigated with plain and surf

174 ent in aqueous detergent solution and at the air-water interface, is preserved in multilayer films of

175 lamethicin helices, oriented parallel to the air/water interface, is presented using synchrotron x-ra

176 ing blocks by dynamic imine chemistry at the air/water interface (Langmuir-Blodgett method).

177 es, whose concentration is stimulated by the air-water interface, leading to formation of the critica

178 re efficiently transferred into the alveolar air-water interface, lowering surface tension to avoid l

179 Furthermore, air-water interface monolayer surface pressure and fluor

180 Consequently, the air/water interface no longer acts as a free surface and

181 Based on the stability of monolayers at the air-water interface, octanoyl-Abeta(16-22) is more amphi

182 The ultrafast oxidation of I(-) by O3 at the air-water interface of microdroplets is evidenced by the

183 tions exposed to 50 ppbv O3 can occur at the air-water interface of sea spray, followed by their tran

184 preferential accumulation of E. coli at the air-water interface of the bubble leads to enhanced toxi

185 of there being a surfactant monolayer at the air-water interface of thin, cryo-EM specimens has been

186 ures of phospholipids and cholesterol at the air-water interface often exhibit coexisting liquid phas

187 apped phospholipid bilayer deposited from an air-water interface onto glass substrates, was investiga

188 In the vadose zone, air-water interfaces play an important role in particle

189 t quantum mechanical calculations on a model air-water interface predict that such event is hindered

190 and a hexadecyl amide of glycine (2) at the air-water interface produces a single dipeptide product

191 alis cells seemed to prefer to attachment at air/water interface rather than sand surface, while E. c

192 9% increases in arsenic concentration at the air-water interface respectively indicating that the muc

193 herms of C18- and C20-sphingosines spread at air/water interfaces reveal unique interfacial propertie

194 n situ UV-vis spectra of the polymers at the air-water interface revealed different behavioral detail

195 apid increases in pore water content such as air-water interface scouring and thin film expansion are

196 le is the hydrophobins, whose aggregation at air-water interfaces serves to create robust protein coa

197 products of AH(2) ozonolysis at the relevant air-water interface shift from the innocuous dehydroasco

198 ospholipids (PPL) from calf surfactant at an air/water interface, surface pressures (pi) reach and su

199 electrostatic energy of lipid domains at the air-water interface, taking account of dipole-dipole rep

200 as a higher propensity to be adsorbed on the air-water interface than to be dissolved in the bulk.

201 nonrandom orientations against the extended air-water interface that exists for a short time before

202 Dry and wet cycles introduce moving air-water interfaces that can scour bacteria from grain

203 yielding a no-slip boundary condition on the air-water interface (the "plastron") for surfactant conc

204 urier transform infrared measurements at the air-water interface, the conformation of PBLA in the mon

205 When they are spread at an air/water interface, the limiting area and the collapse

206 ide secondary structure in monolayers at the air/water interface, the physical state that best approx

207 ity of pulmonary surfactant monolayers at an air/water interface, the studies reported here compared

208 In a monolayer at an air-water interface, these lipids have miscibility trans

209 ng functional nonamphiphilic molecules to an air-water interface through inclusion in a well-defined

210 phenylalkane guests, can be generated at the air-water interface through synergistic structural enfor

211 occurs at the 1,2 carbon-carbon bond at the air-water interface through the formation of (1) an ozon

212 II) phase could hasten lipid transfer to the air-water interface through unstable transition intermed

213 stigated under drainage conditions, with the air-water interface tracked using dyed water and an imag

214 The shrinkage left a large portion of the air-water interface uncovered with lipid molecules.

215 scible liquids in monolayer membranes at the air-water interface under specified conditions of temper

216 e monolayer behavior has been studied at the air-water interface under various subphase conditions.

217 energy dissipation of water molecules at the air-water interface using femtosecond two-color IR-pump/

218 ed experimental and theoretical study of the air-water interface using surface-selective heterodyne-d

219 The arsenic concentration at the air-water interface was measured after equilibration.

220 e spreading of lipid from this system to the air-water interface was rapid at 37 degrees C but slow a

221 rnal reflection infrared spectroscopy at the air-water interface was used to study the influence on p

222 spontaneous formation of the NP film at the air/water interface was due to the minimization of the s

223 The precursor film formed at the air/water interface was heated at 900 degrees C and tran

224 The lateral mobility of Tempo at the air/water interface was measured electrochemically in th

225 e insertion of the surfactant lipids into an air/water interface, we measured the effect of lysophosp

226 rescence microscopy of the monolayers at the air-water interface were complemented with atomic force

227 surfactant (LS) and albumin compete for the air-water interface when both are present in solution.

228 ular structure information from films at the air/water interface where protein adsorption to LPS mono

229 particles then spontaneously migrate to the air/water interface, where they self-assemble, forming a

230 Unlike for the air/water interface, wherein repartitioning of the solve

231 is markedly different from O-H bonds at the air-water interface, which are less heterogeneous, and i

232 Ozone exhibits an affinity for the air-water interface, which modifies its UV and visible l

233 xchange in the antiparallel structure at the air/water interface, which is consistent with the existi

234 benzene, toluene, and anisole) react at the air-water interface with increasing O3(g) during tauc ap

235 brain are investigated as monolayers at the air-water interface with isotherms, fluorescence microsc

236 eared to adopt alpha-helical structure at an air/water interface with a molecular area of 164 A(2) at

237 atile organic compound (formaldehyde) at the air/water interface with explicit description of its gro

238 , formaldehyde exhibits a preference for the air/water interface with respect to the bulk, roughly by

239 to form moderately stable monolayers at the air-water interface, with a collapse pressure that almos

240 ic evidence of peptide bond formation at the air-water interface, yielding a possible mechanism provi