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1 ric acid at the surface of liquid water (the air-water interface).
2 muir films was systematically studied at the air-water interface.
3 of a sequence-specific peptoid polymer at an air-water interface.
4 h and polycrystalline circular assemblies on air-water interface.
5 ne photolysis by UV and visible light at the air-water interface.
6 yers containing Gb3 were investigated at the air-water interface.
7 ion selectively forming peptide bonds at the air-water interface.
8 ge bonded and transported the arsenic to the air-water interface.
9 gh physicochemical processes at and near the air-water interface.
10 tides leads to enriched fibrillization at an air-water interface.
11 urface of water, and quickly dive across the air-water interface.
12 We show that the unfolded regions face the air-water interface.
13 had the largest force due to pinning of the air-water interface.
14 ugh an unusual monolayer intermediate at the air-water interface.
15 loosely packed or arrested structures on the air-water interface.
16 sembly of beta-sheet-forming peptides at the air-water interface.
17 its ability to form continuous layers at the air-water interface.
18 nd the two-dimensional melting in MLF at the air-water interface.
19 s consistent with its role in stabilizing an air-water interface.
20 nd orientation alignment of nanowires at the air-water interface.
21 ecome surface active and are enriched at the air-water interface.
22 splay a unique biolocomotion strategy at the air-water interface.
23 nolayer containing the receptor GM(1) at the air-water interface.
24 y oriented within Langmuir monolayers at the air-water interface.
25 ent of the QDs in the monolayer films at the air-water interface.
26 ineer the 2D self-assembly of the QDs at the air-water interface.
27 fluorescence microscopy of monolayers at the air-water interface.
28 "reservoirs" of fluid phase adjacent to the air-water interface.
29 a dense band at a certain distance from the air-water interface.
30 rm of dSP-C is not surface-associated at the air-water interface.
31 l iron-nickel cyanide-bridged network at the air-water interface.
32 and SP-C in lipid-protein monolayers at the air-water interface.
33 triple-stranded beta-sheet monolayer at the air-water interface.
34 ble into two-dimensional crystallites at the air-water interface.
35 ter ions toward the features observed at the air-water interface.
36 haracteristic of an edge-on structure at the air-water interface.
37 emplating method (template-inhibition) at an air-water interface.
38 from the appropriate monolayer phase at the air-water interface.
39 spholipid monolayers was investigated at the air-water interface.
40 , both single compounds and mixtures, at the air-water interface.
41 it adsorption of pulmonary surfactant to the air-water interface.
42 neous monolayers at constant pressure at the air-water interface.
43 e when spread on top of a urease film at the air-water interface.
44 is either nonexistent or inaccessible at an air-water interface.
45 layer of monodendrons during collapse at the air-water interface.
46 an iminodiacetate-Cu(II) lipid spread at the air-water interface.
47 e of domain sizes in lipid monolayers at the air-water interface.
48 that can spread rapidly from solution to the air-water interface.
49 rged species to exhibit a propensity for the air-water interface.
50 id, overcomes persistent denaturation at the air-water interface.
51 ace ligands and subsequently assembled at an air-water interface.
52 fic adsorption of guanidinium cations to the air-water interface.
53 n of PFOS due to its higher affinity for the air-water interface.
54 e presence of hydroxyl radicals (OH.) at the air-water interface.
55 th scale beyond which the flow mobilizes the air-water interface.
56 nitric acid and is fully dissociated at the air-water interface.
57 es in the spectra of carboxylic acids at the air-water interface.
58 ic behavior of syn- and anti-CH3 CHOO at the air-water interface.
59 e reactivity of Criegee intermediates at the air-water interface.
60 e, reminiscent of the canonical, hydrophobic air-water interface.
61 favorable exposure of H atoms of H2O at the air-water interface.
62 digestion, both in bulk and adsorbed at the air-water interface.
63 = CH3; and for CH3NH2, R1 = R2 = CH3) at the air-water interface.
64 ine both increase the surface tension at the air-water interface.
65 reaction mechanism of singlet oxygen at the air-water interface.
66 rated compounds by chemical reactions at the air-water interface.
67 id proxy which formed an organic film at the air-water interface.
68 isopropyl methyl groups of l-leucine at the air-water interface.
69 perties of pulmonary surfactant films at the air-water interface.
70 ical force to its molecular monolayer at the air-water interface.
71 ot even capable of forming monolayers at the air-water interface.
72 eracted with anionic lipid monolayers at the air/water interface.
73 ntus, a singly flagellated bacterium, at the air/water interface.
74 he adsorption of the surfactant lipids to an air/water interface.
75 acting on water to produce cavitation at the air/water interface.
76 parated from the solution and floated at the air/water interface.
77 ctivity of volatile organic compounds at the air/water interface.
78 c wrinkled structures when illuminated at an air/water interface.
79 Additional studies were performed at the air/water interface.
80 pid adsorption of pulmonary surfactant to an air/water interface.
81 to the parallel beta-sheet structure at the air/water interface.
82 anced concentrations of selected ions at the air/water interface.
83 the value determined for thiocyanate at the air/water interface.
84 rbles" that remain stable when placed at the air/water interface.
85 itially lie flat on the water surface at the air/water interface.
86 electrolyte ions between bulk water and the air/water interface.
87 metry with line microelectrodes touching the air/water interface.
88 esidue beta-hairpin peptides adsorbed at the air/water interface.
89 ectron hopping in Langmuir monolayers at the air/water interface.
90 onal order in monolayer films in situ at the air/water interface.
91 d peptide secondary structure in situ at the air/water interface.
92 ually exhibit enhanced concentrations at the air/water interface.
93 opropylacrylamide) (PNiPAm) microgels at the air/water interface.
94 ant entropy contribution, in contrast to the air/water interface.
95 ives with SDS for available positions at the air/water interface.
96 e reported out-of-plane reorientation at the air/water interface.
97 central triptycene core are confined at the air/water interface.
98 ete Pythium ultimum that was grown along the air-water interfaces.
99 elementary amphiphilic receptors anchored at air-water interfaces.
100 decyl ether (C(12)E(3)) source droplets over air-water interfaces.
101 es start and run autonomously when placed at air-water interfaces.
102 o the gas phase, and we conclude that at the air-water interface, a lower limit for the rate constant
103 corporation of lipids into monolayers at the air-water interface after collapse is important to the m
104 anges in the amide I spectra of hIAPP at the air/water interface after addition of dipalmitoylphospho
105 because of its enhanced fractionation at the air-water interface and ability to donate electrons.
106 artitioning of hydrophobic proteins into the air-water interface and allows imaging of the foam struc
107 tructural changes to lipid monolayers at the air-water interface and bilayers at the solid-water inte
108 imate that up to 87% of PFOS mass was at the air-water interface and less than 4% at the dodecane-wat
110 the nanodrops is similar to that at the bulk air-water interface and that the hydrogen bonding of int
112 he spacer keeps particles away from both the air-water interface and the graphene oxide surface, prot
113 ionization state of organic molecules at the air-water interface and the related problem of the surfa
114 e suspensions could then be dispersed at the air-water interface and transferred to silicon wafers us
117 ribes a two-dimensional polymerization at an air/water interface and provides, for the first time, di
118 s showed that EPL1 readily self-assembles at air/water interfaces and forms protein layers that can b
119 rties of BUBR1(1-204) and TPR-PP5(16-181) at air/water interfaces and found that both proteins exhibi
120 natural and artificial bodies moving at the air-water interface, and can inform the design of aerial
121 d a highly emissive face-on structure at the air-water interface, and did not form pi-aggregates.
122 udies of the behavior of the polymers at the air-water interface, and of the photophysical properties
123 ides were reconstituted as monolayers at the air-water interface, and their properties, as well as th
124 low foaming, high areas of occupancy at the air/water interface, and weak solid-adsorption and solub
127 dihydrocholesterol and phospholipids at the air-water interface are used to model membranes containi
131 We use the hydrophobic environment of the air-water interface as a favorable venue for peptide bon
132 ze spherical and ellipsoidal particles at an air-water interface as a function of surface coverage.
133 CPA oxidation by OH in the gas-phase, at the air-water interface as well as in the solid phase (dry f
134 the field of 2D polymers synthesized at the air/water interface as it, in principle, allows estimati
135 ree-energy profile for a solute crossing the air-water interface, as well as the thermodynamic cost o
136 s the surface activity of the protein at the air:water interface, as determined by surface tension me
138 ynthetic D-erythro C18-ceramide films at the air-water interface at various surface pressures (pi).
139 of xylem sap plays a key role in stabilizing air-water interfaces at the pits between water- and gas-
140 ine-(leucine)4]4-lysine (KL4), spread at the air/water interface at 25 degrees C and pH 7.2, and its
142 NP BTCs and indicated that attachment to the air-water interface (AWI) occurring during FI was the ke
144 mer formation to be higher and faster at the air-water interface (AWI) than in the bulk (by 14 and ap
145 bibition efficiently released cells from the air-water interface (AWI) that were initially retained u
146 mate of the average PFAS accumulation at the air-water interface (AWI), generally predicted PFAS pore
148 ns are repelled from water/hydrophobe (e.g., air/water) interfaces, both computer simulations and exp
149 tructure of yeast fatty acid synthase at the air-water interface by electron cryo-tomography and sing
150 These polymers were characterized at the air-water interface by Langmuir techniques and found to
152 hus, after the ellipsoids are carried to the air-water interface by the same outward flow that causes
153 nd transport, as particles can attach to the air-water interfaces by action of capillary forces.
154 methods was attributed to saturation of the air/water interface by a DTAB/trianion complex far below
156 erse polystyrene (PS) particle monolayers at air/water interfaces by using our needle tip flow method
157 ., viruses and proteins), the velocity on an air-water interface can be as large as approximately 47
158 roscopy of phase-separated monolayers at the air-water interface can be generated by the selective ad
160 mixed with cholesterol in a monolayer at an air-water interface, coexisting 2-dimensional liquid pha
161 protein and lipid-protein monolayers at the air-water interface confirmed that the residual dSP-C he
163 the non-equilibrium crystalline phase on the air-water interface could be explained with a model that
164 water interfacial systems indicated that the air-water interface could markedly lower the free-energy
168 visualized colloids interacting with moving air-water interfaces during capillary fringe fluctuation
170 whey and acid bovine whey were preserved at air water interface even after a heat treatment at 90 de
171 tering that nanoparticle membranes formed at air/water interfaces exhibit a small but significant app
172 onsible for stability of microbubbles at the air-water interface, facilitating its surfactant behavio
174 e transition temperatures and behavior at an air-water interface for this series are similar to phosp
176 the bordered pit chamber such that a convex air-water interface forms at the entrance into the pit c
177 es the water strider poised to penetrate the air-water interface from below, which appears impossible
178 e oxidation of the complex monolayers at the air-water interface from two potent oxidizers hydroxyl r
180 likely create a small negative charge at the air-water interface, generating an electric double layer
182 eramide (GM(1)), in a lipid monolayer at the air-water interface has been studied utilizing grazing i
183 alysis of the self-assembly mechanism at the air/water interface has been carried out, and the propos
186 Molecular areas of soluble films at the air/water interface have traditionally been calculated b
187 surfaces models, based on LPS monolayers at air-water interfaces, have so far dealt only with rough
190 (i) they self assemble into monolayers at an air/water interface; (ii) the monolayers are dominated b
192 e to photochemical reactions occurring at an air-water interface in presence of model saturated long
193 s study, the micron-scale Haines jump of the air-water interface in rough fractures was investigated
196 c-hydrophilic interfaces, represented by the air-water interface in vitro and diverse heterogeneous i
197 ct quantification of PFAS mass sorbed at the air-water interface in water films were used to evaluate
198 g self-assembly of protein aggregates at the air-water interface in which initial foam formation is f
199 ed by hydrophobic-hydrophilic interfaces (an air-water interface in-vitro or membranes in-vivo).
203 chemicals to calibrate mass transfer at the air/water interface in a fugacity-based multimedia model
205 tant, a lipid/protein complex that lines the air/water interface in the mammalian lung, functions to
207 re we measure the surface deformation at the air-water interface induced by continuous and pulsed las
208 lenges such as inconsistent ice thicknesses, air-water interface interactions and preferred particle
209 nt to visible light, we demonstrate that the air-water interface interacts strongly with visible ligh
217 ganization of bacteria in thin films or near air-water interfaces is strongly impacted by a purely ph
220 compressional instability of particle-laden air/water interfaces is investigated with plain and surf
221 ent in aqueous detergent solution and at the air-water interface, is preserved in multilayer films of
222 lamethicin helices, oriented parallel to the air/water interface, is presented using synchrotron x-ra
224 es, whose concentration is stimulated by the air-water interface, leading to formation of the critica
225 re efficiently transferred into the alveolar air-water interface, lowering surface tension to avoid l
226 IO(x) (x = 2 and 3)-IONO(2)] dynamics at the air-water interface modeled by a water droplet of 191 wa
229 Based on the stability of monolayers at the air-water interface, octanoyl-Abeta(16-22) is more amphi
231 The ultrafast oxidation of I(-) by O3 at the air-water interface of microdroplets is evidenced by the
232 tions exposed to 50 ppbv O3 can occur at the air-water interface of sea spray, followed by their tran
233 preferential accumulation of E. coli at the air-water interface of the bubble leads to enhanced toxi
234 of there being a surfactant monolayer at the air-water interface of thin, cryo-EM specimens has been
236 ures of phospholipids and cholesterol at the air-water interface often exhibit coexisting liquid phas
237 apped phospholipid bilayer deposited from an air-water interface onto glass substrates, was investiga
240 on of a macroscopic, gelatinous layer at the air/water interface, possibly related to tau phase separ
241 t quantum mechanical calculations on a model air-water interface predict that such event is hindered
242 and a hexadecyl amide of glycine (2) at the air-water interface produces a single dipeptide product
243 alis cells seemed to prefer to attachment at air/water interface rather than sand surface, while E. c
244 9% increases in arsenic concentration at the air-water interface respectively indicating that the muc
245 herms of C18- and C20-sphingosines spread at air/water interfaces reveal unique interfacial propertie
246 n situ UV-vis spectra of the polymers at the air-water interface revealed different behavioral detail
247 H from the water molecules that straddle the air-water interface reveals that the second solvation sh
248 apid increases in pore water content such as air-water interface scouring and thin film expansion are
249 le is the hydrophobins, whose aggregation at air-water interfaces serves to create robust protein coa
250 products of AH(2) ozonolysis at the relevant air-water interface shift from the innocuous dehydroasco
251 llutants, their spontaneous formation at the air-water interface should have important implications i
252 ospholipids (PPL) from calf surfactant at an air/water interface, surface pressures (pi) reach and su
253 MOFs were employed in a microbubble-assisted air-water interface system for nitrogen fixation under a
254 electrostatic energy of lipid domains at the air-water interface, taking account of dipole-dipole rep
255 as a higher propensity to be adsorbed on the air-water interface than to be dissolved in the bulk.
256 nonrandom orientations against the extended air-water interface that exists for a short time before
258 yielding a no-slip boundary condition on the air-water interface (the "plastron") for surfactant conc
259 urier transform infrared measurements at the air-water interface, the conformation of PBLA in the mon
261 ide secondary structure in monolayers at the air/water interface, the physical state that best approx
262 ity of pulmonary surfactant monolayers at an air/water interface, the studies reported here compared
265 ng functional nonamphiphilic molecules to an air-water interface through inclusion in a well-defined
266 phenylalkane guests, can be generated at the air-water interface through synergistic structural enfor
267 occurs at the 1,2 carbon-carbon bond at the air-water interface through the formation of (1) an ozon
268 II) phase could hasten lipid transfer to the air-water interface through unstable transition intermed
269 stigated under drainage conditions, with the air-water interface tracked using dyed water and an imag
271 scible liquids in monolayer membranes at the air-water interface under specified conditions of temper
272 e monolayer behavior has been studied at the air-water interface under various subphase conditions.
273 en bond-driven HIO(3)-IONO(2) complex at the air-water interface undergoes deprotonation and exists a
274 energy dissipation of water molecules at the air-water interface using femtosecond two-color IR-pump/
275 ed experimental and theoretical study of the air-water interface using surface-selective heterodyne-d
276 e to tremendous impedance mismatch at stable air/water interfaces, viz., the Cassie-Baxter state is d
278 e spreading of lipid from this system to the air-water interface was rapid at 37 degrees C but slow a
279 rnal reflection infrared spectroscopy at the air-water interface was used to study the influence on p
280 spontaneous formation of the NP film at the air/water interface was due to the minimization of the s
283 e insertion of the surfactant lipids into an air/water interface, we measured the effect of lysophosp
284 rescence microscopy of the monolayers at the air-water interface were complemented with atomic force
285 oncentrations of PFOA, PFOS, and FOSA at the air-water interface were from 2 to 16 times greater than
286 surfactant (LS) and albumin compete for the air-water interface when both are present in solution.
287 ular structure information from films at the air/water interface where protein adsorption to LPS mono
288 particles then spontaneously migrate to the air/water interface, where they self-assemble, forming a
290 is markedly different from O-H bonds at the air-water interface, which are less heterogeneous, and i
292 xchange in the antiparallel structure at the air/water interface, which is consistent with the existi
293 benzene, toluene, and anisole) react at the air-water interface with increasing O3(g) during tauc ap
294 brain are investigated as monolayers at the air-water interface with isotherms, fluorescence microsc
295 eared to adopt alpha-helical structure at an air/water interface with a molecular area of 164 A(2) at
296 atile organic compound (formaldehyde) at the air/water interface with explicit description of its gro
297 , formaldehyde exhibits a preference for the air/water interface with respect to the bulk, roughly by
298 to form moderately stable monolayers at the air-water interface, with a collapse pressure that almos
299 nd 6:2 FTS was retarded by adsorption at the air-water interface, with greater retention of PFOS due
300 ic evidence of peptide bond formation at the air-water interface, yielding a possible mechanism provi