ライフサイエンスコーパス: Langmuir

1 Langmuir asserted that its proper use in public health m

2 Langmuir binding isotherms predicted the maximum amount

3 Langmuir binding isotherms were applied to determine qua

4 Langmuir coefficients varied with sorbent surface chemis

5 Langmuir isotherm theory conceptualized saturable surfac

6 Langmuir isotherms provided better fits to equilibrium d

7 Langmuir maximum sorption capacities (Qmax) for N2O on t

8 Langmuir monolayer model (q(m) = 32.4 mg/g, R(L) = 0.99

9 Langmuir monolayers (monolayers of insoluble molecules f

10 Langmuir, Freundlich, Scatchard and D-R (Dubinin-Radushk

11 Langmuir-based kinetics, which describe alkanethiolate a

12 Langmuir-Blodgett and Langmuir-Schaeffer deposition and

13 Langmuir-Blodgett films of metallosurfactants were used

14 Langmuir-Schaefer film deposition was used to deposit na

15 Langmuir-Wilhelmy surface balance, fluorescence microsco

16 e determined using a Biacore SPR device (1:1 Langmuir binding model).

17 10(-4) M) using SPR by fitting data to a 1:1 Langmuir interaction model.

18 protein immobilization were fitted to a 1:1 Langmuir-type model, yielding K(LM) = 2.5 x 10(5) M(-1)

19 xide (ITO) directly from Nafion-[Ru(bpy)3]2+ Langmuir films assembled at the water-air interface.

20 tions of endotoxin that are less than 10(-5) Langmuir, are not due to adsorbate-induced changes in th

21 A Langmuir adsorption coefficient of 1.6 x 10(7) M(-1) was

22 A Langmuir adsorption model was used to derive quantitativ

23 A Langmuir isotherm model was applied to determine the bin

24 A Langmuir isotherm model yields KD=(2.1+/-1.1)muM as the

25 A Langmuir second-order kinetic law is applied to regulate

26 ecedented five-step adsorption process and a Langmuir surface area of 2670 m2/g.

27 Assuming a Langmuir adsorption isotherm, the dissociation constant

28 In addition, by assuming a Langmuir-type adsorption isotherm to measure the initial

29 of melatonin concentration, is well fit by a Langmuir adsorption isotherm.

30 face pressure measurements and analyzed by a Langmuir competitive adsorption model.

31 orb to a cationic lipid template formed by a Langmuir monolayer of DPTAP (1,2-dihexadecanoyl-3-trimet

32 rlying calmodulin/channel interactions, by a Langmuir relation (individually transformed Langmuir ana

33 into a biomimetic environment provided by a Langmuir-Blodgett (LB) film of arachidic acid (AA).

34 inding of pamidronate is well described by a Langmuir-like isotherm, from which we deduce an approxim

35 Here authors develop a Langmuir-Blodgett method to organize charge transfer mol

36 It exhibits a Langmuir surface area of 1470 m(2) g(-1), and its struct

37 ct generation, all Au nanoparticles follow a Langmuir-Hinshelwood mechanism but with heterogeneous re

38 ible by application of salts, and followed a Langmuir adsorption isotherm dependent on the particle s

39 sity showed an increasing trend, following a Langmuir absorption function (R(2) = 0.94).

40 Binding between both follows a Langmuir adsorption type model and creates a surface pot

41 n the equilibrium adsorption isotherm from a Langmuir type to a Freundlich type with much higher adso

42 are deposited on lung surfactant films in a Langmuir trough.

43 ted on a fluid is compressed uniaxially in a Langmuir trough.

44 ft-squeezing technique and were studied in a Langmuir trough.

45 tion of electrical current was observed in a Langmuir-Schaefer monolayer of fullerene-bis[ethylthio-t

46 understand PFOS association into the MIP, a Langmuir binding model was developed based on the change

47 Analysis of the results in terms of a Langmuir model for binding to a surface suggests that th

48 ture and surface pressure-area isotherm of a Langmuir monolayer (LM) on a water subphase as a functio

49 typically studied on the planar surface of a Langmuir trough, even though most physiological interfac

50 dsorption studies of PCN-14 at 77 K reveal a Langmuir surface area of 2176 m2/g and a pore volume of

51 that a Freundlich-based model, rather than a Langmuir-based model, described perfluorooctanoic acid (

52 Passage of the supported oil films through a Langmuir monolayer is shown to lead to quantitative tran

53 suggests that N2 O is not produced through a Langmuir-Hinshelwood mechanism; rather, its formation is

54 Fitting the integrated response to a Langmuir isotherm yielded a calculated binding constant

55 ith the concentration and can be fitted to a Langmuir isotherm.

56 ic rate law for O2 disappearance points to a Langmuir-Hinshelwood surface-based reaction mechanism po

57 acity of nanomaghemite was evaluated using a Langmuir isotherm model, and a diffuse double layer surf

58 ing affinity among the 3 amelogenins using a Langmuir model for protein adsorption.

59 Using a Langmuir monolayer insertion assay, two mPEs are found t

60 (FC) on meibomian lipid films (MLF) using a Langmuir trough (LT) and a Brewster angle microscope (BA

61 e.e.g has been modelled successfully using a Langmuir-like adsorption isotherm that incorporates the

62 (18:1, 24:1) have been characterized using a Langmuir-type film balance.

63 ere evaluated and were found to adsorb via a Langmuir model and to have binding capacities in the ord

64 n as expected for reactions proceeding via a Langmuir-Hinshelwood mechanism.

65 ed by fitting the adsorption profiles with a Langmuir equation and, in the case of single-charged sur

66 Adsorption processes were modeled with a Langmuir isotherm, and detection of other neurochemicals

67 n of p40(phox) protein (p40(phox)-PX) with a Langmuir monolayer of a mixture of SOPC (1-stearoyl-2-ol

68 COF-320 exhibits permanent porosity with a Langmuir surface area of 2400 m(2)/g and a methane total

69 Alexander Langmuir, head of the Epidemiology Branch, redefined sur

70 In 1949, Alexander Langmuir became the first chief epidemiologist at the Co

71 ess has been made with directed assembly and Langmuir-Blodgett approaches, it is unclear whether thes

72 vealed a type I isotherm, indicating BET and Langmuir surface areas of 1810 and 2040 m(2)/g, respecti

73 c model envelope using Langmuir-Blodgett and Langmuir-Schaefer methods is now reported.

74 Langmuir-Blodgett and Langmuir-Schaeffer deposition and self-assembly techniqu

75 igated by adsorption/elution experiments and Langmuir isotherms.

76 ion was best described by the Freundlich and Langmuir isotherm, respectively, with a maximum As(V) up

77 linear isotherm models, e.g., Freundlich and Langmuir models, are not.

78 The Langmuir, Freundlich, and Langmuir-Freundlich isotherms were fitted to the epitope

79 gmuir specific surface area >1500 m(2)/g and Langmuir constant (k(L)) > 0.1 to adsorb water vapor and

80 Ns are sprayed onto layer-by-layer (LbL) and Langmuir-Blodgett (LB) films, and samples are fabricated

81 Using Brewster angle microscopy and Langmuir monolayer compression isotherms, we show that t

82 ohol systems using infrared spectroscopy and Langmuir trough measurements indicate that precisely tho

83 Pulsating bubble surfactometry and Langmuir-Wilhelmy surface balance studies showed that al

84 mple, MOF-210 has Brunauer-Emmett-Teller and Langmuir surface areas of 6240 and 10,400 square meters

85 g the binding data to both the Hill-Waud and Langmuir adsorption isotherm equations.

86 lope that is proportional to the appropriate Langmuir adsorption coefficient.

87 d chemical stability with high surface area (Langmuir surface area of 782 m(2)/g(-1)) comparable to o

88 arbon chain suggests that mechanisms such as Langmuir-Hinshelwood, Eley-Rideal, and Diels-Alder might

89 med at the surface of water), and associated Langmuir-Blodgett/Schaefer monolayers prepared by transf

90 Complete domain registration between Langmuir-Blodgett and Schaefer monolayer domains was obs

91 romatography was derived in the case of a bi-Langmuir adsorption isotherm model.

92 we could calculate the parameters of the bi-Langmuir adsorption model for phenol on a column packed

93 e best adsorption isotherm models are the bi-Langmuir and the tetra-Langmuir isotherms for XTerra and

94 data for phenol are best modeled with the bi-Langmuir and the tri-Langmuir isotherm models for Kromas

95 1.43 x 10(5) s(-1)) than that of bimolecular Langmuir-Hinshelwood (L-H) pathway (4.29 s(-1)).

96 ilayers, deposited via the Langmuir-Blodgett/Langmuir Schaefer methodology, was investigated by z-sca

97 silica supports using the Langmuir-Blodgett/Langmuir-Schaeffer technique, which allows precise contr

98 tion of microporous domains characterized by Langmuir sorption in local equilibrium with a minority c

99 omain of synaptotagmins 1/2 and confirmed by Langmuir monolayer, surface plasmon resonance, and circu

100 Data were well described by Langmuir isotherms with gamma(max)(Ca(2+)) of 9.5 +/- 0.

101 hemical sciences, and is well exemplified by Langmuir's concept of isovalency, in which 'two molecula

102 s were studied at the air-water interface by Langmuir-Blodgett assembly.

103 interface of model membranes represented by Langmuir phospholipid monolayers and Aerosol-OT (AOT) re

104 ows a highly porous material with calculated Langmuir and BET surface areas of 1320 and 1270 m2 g(-1)

105 athode to the level far surpassing the Child-Langmuir's space-charge-limited emission.

106 sed tethered polymer supports and a combined Langmuir-Blodgett/vesicle fusion (LB/VF) technique to bu

107 On the basis of competitive Langmuir isotherms, if the eluent anion is more strongly

108 trument enables the collection of a complete Langmuir binding curve on a single sensor surface.

109 gle Pt atoms cannot occur via a conventional Langmuir-Hinshelwood scheme (L-H scheme) which requires

110 of the charged species are more conventional Langmuir isotherms.

111 Unlike the conventional Langmuir-Hinshelwood (L-H) mechanism, the CO molecule ad

112 Alexander D. Langmuir is credited with articulating the concept of di

113 e measured and modeled by the time dependent Langmuir equation.

114 In this paper, I describe Langmuir's redefinition of surveillance.

115 used in these experiments with two different Langmuir adsorption coefficients, K(A1) = 4.4 x 10(8) M(

116 (3.0 +/- 0.5) x 107 M-1 using an equilibrium Langmuir model.

117 The estimated Langmuir affinity constant (K(L)) was 21 +/- 5 muM(-1) P

118 field theory modeling, from which we exclude Langmuir adsorption.

119 Brunauer-Emmett-Teller (BET) theory extended Langmuir's ideas to multilayer adsorption.

120 profile analysis tensiometry (Gibbs films), Langmuir monolayers and microbubble experiments.

121 Binding isotherm followed Langmuir isotherm model of monolayer adsorption with a m

122 All four species followed Langmuir adsorption isotherms.

123 inium, and thiouronium units that all formed Langmuir monolayers.

124 The pronounced deviation from Langmuir adsorption behavior is greater for longer duple

125 Furthermore, Langmuir-Blodgett films of MOSCs were prepared and the u

126 rmined by fitting isotherms to a generalized Langmuir-type equation.

127 ling of the experimental data, based on Hill-Langmuir adsorption characteristics, suggests that these

128 It has been shown that the hyperbolic Langmuir isotherm captures the shape of the signal respo

129 peculiar features inconsistent with an ideal Langmuir-like behavior.

130 l-organic supercontainer (MOSC) molecules in Langmuir films was systematically studied at the air-wat

131 or X-ray reflection of the same proteins in Langmuir monolayers can be more informative than the iso

132 ew type of HX MS measurement that integrates Langmuir monolayers.

133 pectrometry (MS) measurement that integrates Langmuir monolayers.

134 imine chemistry at the air/water interface (Langmuir-Blodgett method).

135 ned to interleave on an aqueous surface into Langmuir-Blodgett (LB) monolayers containing a two-dimen

136 I joined Langmuir as assistant chief in 1955 and was appointed ch

137 itous in superfluids, liquid crystals (LCs), Langmuir monolayers, and Bose-Einstein condensates.

138 To model its outer leaflet, Langmuir monolayers and cushioned supported bilayers wer

139 ructural features of water confined in lipid Langmuir monolayers are revealed.

140 ry force lithography, colloidal lithography, Langmuir-Blodgett lithography) (116 references).

141 tionship (pp-LFER) is able to predict median Langmuir binding constants for graphite, charcoal, and D

142 orbate-specific binding constant, the median Langmuir binding constant, and two global sorbent parame

143 and the pp-LFER below the cutoff, the median Langmuir binding constants can be predicted with a root-

144 ent, as a plateau is observed for the median Langmuir binding constants of larger molecular volume so

145 isotherm parameters, specifically the median Langmuir binding constants, KL, obtained utilizing the s

146 ty of these large compounds and their median Langmuir binding constants.

147 bination of in situ atomic force microscopy, Langmuir trough techniques, and vesicle permeability ass

148 he properties of circular domains in a mixed Langmuir monolayer at thermodynamic equilibrium.

149 numerically and incorporated into a modified Langmuir scheme, allowing kinetic suppression of hybridi

150 Here, we report a modified Langmuir-Blodgett method to organize two-dimensional mol

151 explain these results, we explored modified Langmuir-Hinshelwood type pathways that have been propos

152 avior of Au/thiol self-assembled monolayers, Langmuir-Blodgett films, and porphyrin molecules chemiso

153 pproach relies on formation of monomolecular Langmuir films (LFs) at the interphase of aqueous barium

154 Overall, the HX MS Langmuir monolayer method provided new and meaningful co

155 The HX MS Langmuir monolayer method provides new and meaningful in

156 d by lipid association, we applied the HX MS Langmuir monolayer method to myrNef associated with mono

157 the adsorption data to the appropriate multi-Langmuir adsorption isotherm model, were analyzed and co

158 This information is used in a multisite Langmuir model, augmented with a Bragg-Williams model fo

159 A stepwise multisite Langmuir model was developed to simulate the stepwise ad

160 dyl)ruthenium(II), [Ru(bpy)3]2+, into Nafion Langmuir-Schaefer (LS) films is described.

161 We propose a simple non-Langmuir kinetic model accounting for an enhanced electr

162 his, several simplifications to a log-normal Langmuir (LNL) isotherm model with 3n parameters were ex

163 ing the single-chemical parameter log-normal Langmuir isotherm developed in the accompanying work.

164 lectrodes was investigated and found to obey Langmuir adsorption isotherm characteristics.

165 It was found that uranyl sorption obeyed Langmuir isotherm model giving a maximum U(VI) membrane

166 KA), a galactose-specific lectin, and AFM of Langmuir-Blodgett deposited GalCer/DLPC supported lipid

167 Analysis of Langmuir isotherms and microstructural characterization

168 the recording of isotherms of compression of Langmuir films for temperatures above and below the gel

169 h an alkyl tail facilitates the formation of Langmuir-Blodgett (LB) monolayers.

170 Finally, measurement of Langmuir isotherms was employed to provide classical evi

171 s of the PS film have relied on the model of Langmuir monolayers.

172 What makes these and many other of Langmuir's innovations so remarkable is their continued

173 ts of the studies relating to preparation of Langmuir-Blodgett (LB) monolayers of tri-n-octylphosphin

174 is utilized to characterize the response of Langmuir-Blodgett (LB) multilayers under the bombardment

175 of electron beam exhibits outward spirals of Langmuir turbulence and the center region of the spirals

176 oid nanoparticles can be modeled in terms of Langmuir-type adsorption isotherms (Hill model).

177 /Schaefer monolayers prepared by transfer of Langmuir films to the surfaces of solids, are widely use

178 nd facile procedure that permits transfer of Langmuir monolayers from the surface of water onto micro

179 Our use of Langmuir films provides a novel approach to access tunab

180 urves that may be fitted to a model based on Langmuir adsorption isotherms and simple analytical expr

181 0 was 24.2, 18.8, and 15.1 mg g(-1) based on Langmuir isotherm.

182 Based on Langmuir model, the adsorption capacity of P-Tris nanofi

183 roximate agreement with predictions based on Langmuir's estimated DeltaG(f) degrees , although the pr

184 orporation into Layer-by-Layer assemblies or Langmuir-Blodgett films and hierarchical self-assembly o

185 (PL) spectroscopy and exhibited first-order Langmuir adsorption behavior.

186 ion is, however, consistent with first-order Langmuir adsorption kinetics at low surface coverages.

187 -11, demonstrated their permanent porosity (Langmuir surface area = 1,810 m(2)/g), high thermal stab

188 de capped cadmium selenide quantum dots (QD) Langmuir monolayer.

189 oherent emission is maintained by repetitive Langmuir collapse driven by the nonlinear evolution of a

190 amped by electrons and reexcites small-scale Langmuir waves; this process closes a feedback loop that

191 by the Cassini Radio and Wave Plasma Science Langmuir Probe, the Ion and Neutral Mass Spectrometer an

192 to linear peptide epitopes followed a simple Langmuir model.

193 In particular, according to the simple Langmuir isotherm, all probes should saturate at the sam

194 been made for He, CO2, and N2 across single Langmuir-Blodgett (LB) bilayers derived from 1,2,4,5-tet

195 We first incorporated a standard one-site Langmuir binding model describing probe-analyte interact

196 r studies demonstrated that the 1:1 one-site Langmuir model accurately described the observed respons

197 e of macrospot AIR arrays, either a two-site Langmuir model or a Sips isotherm better described the b

198 ons, including subphase replacement, in situ Langmuir-Blodgett transfer, and real-time surface tensio

199 oupled with a dynamic, triple-mode sorption (Langmuir, Henry, and pooling modes) model employed in th

200 zation exchange model, assuming steady-state Langmuir adsorption under hyperpolarized gas flow condit

201 vapor deposited onto a C18 cadmium stearate Langmuir-Blodgett monolayer supported on Au, SiO2, or Pt

202 ching reaction was modeled with a three-step Langmuir-Hinshelwood mechanism.

203 ), and phosphatidylcholine (PC) on supported Langmuir-Blodgett films are investigated as a mimic of t

204 erm models are the bi-Langmuir and the tetra-Langmuir isotherms for XTerra and Resolve, respectively.

205 The Langmuir isotherm describes the adsorption data well and

206 The Langmuir term represents the adsorption of the analyte o

207 The Langmuir waves are modulated by solitary waves in the li

208 The Langmuir, Freundlich, and Langmuir-Freundlich isotherms

209 The Langmuir-Freundlich isotherm study revealed that M-75 ha

210 The Langmuir-Hinshelwood model fits the photocatalytic inact

211 The Langmuir-Hinshelwood model was applied to the chemical p

212 From the N(2) isotherm for MOP-101, the Langmuir and BET surface areas of MOP-101 were calculate

213 are based on the pseudo-second-order and the Langmuir isotherm models, respectively.

214 tor sites were additionally evaluated by the Langmuir adsorption model.

215 is complicated by limitations imposed by the Langmuir binding isotherm and mass transport, for surfac

216 ions was nonlinear and best described by the Langmuir isotherm.

217 behavior that is not well represented by the Langmuir model; therefore, calorimetric data should be u

218 ing from 150 to above 1000 kilometers by the Langmuir Probe and Wave instrument on the Mars Atmospher

219 Pt-SWNTs prepared by the Langmuir-Blodgett (LB) technique exhibited the highest P

220 ynthesis, therefore, does not proceed by the Langmuir-Hinshelwood mechanism often invoked.

221 d-relevant PFOS and PFOA concentrations, the Langmuir-based model underpredicted interfacial uptake b

222 The chromium adsorption nicely fits the Langmuir isotherm model, and the removal of Cr(VI) from

223 The adsorption is shown to follow the Langmuir isotherm with P(1/2)(298K) = 3200 Torr.

224 all tested odorants are shown to follow the Langmuir model for ligand-receptor interactions.

225 The reaction is demonstrated to follow the Langmuir-Hinshelwood mechanism, known to prevail for het

226 range from 5 to 250 mug mL(-1) following the Langmuir adsorption model.

227 The absorption of Cs(+) by KMS-1 follows the Langmuir model with a high exchange capacity of 226(4) m

228 ies of around 14-15 kJ/mol obtained from the Langmuir adsorption model.

229 ty and sorption affinity parameters from the Langmuir, Freundlich, and Polanyi-Dubinin-Manes (PDM) mo

230 ree distinct methods of preparation: (i) the Langmuir-Blodgett (LB) technique, involving the transfer

231 centers, was obtained by ECS and used in the Langmuir adsorption model to obtain the affinity constan

232 ing the orientation of MOSC molecules in the Langmuir films.

233 ion indicate that preexisting domains in the Langmuir-Blodgett monolayer induce the formation of comp

234 on the J55 and N80 steel surface obeyed the Langmuir adsorption isotherm.

235 sorption isotherm is higher than that of the Langmuir adsorption isotherm.

236 te density and the standard deviation of the Langmuir binding constant were employed.

237 (5) M(-1) was calculated on the basis of the Langmuir isotherm equation.

238 rticle is determined by interpolation of the Langmuir isotherm for pMA.

239 The validity of the Langmuir isotherm suggests monolayer sorption, which can

240 with the Sips model, a generalization of the Langmuir model that allows for multiple binding energies

241 manner that satisfies the assumptions of the Langmuir model.

242 cterization of the interfaces outside of the Langmuir trough, (iii) can be prepared with prescribed a

243 n intraparticle diffusion model based on the Langmuir isotherm adequately predicted column results wh

244 observed binding rate constant, based on the Langmuir kinetic model, was determined to be 0.15 min-1.

245 The proposed model is based on the Langmuir-Hinshelwood-Hougen-Watson (L-H-H-W) postulates

246 the Freundlich and dubinin-radushkevich, the Langmuir isotherm model showed the best fit, with a maxi

247 It was shown that the Langmuir adsorption isotherm recapitulates a general tre

248 action shows a behavior corresponding to the Langmuir adsorption theory with a Limit of Detection (LO

249 replaced water mass is mainly related to the Langmuir adsorption volume of CO2 and increases as the C

250 The data fitted well to the Langmuir model describing a 1:1 interaction.

251 oth with and without treatment fitted to the Langmuir model, and the sorption rate data well fitted t

252 orption of the adsorbents fitted well to the Langmuir model, and the sorption rate fitted well to a p

253 and the adsorption isotherm conformed to the Langmuir model, implying that the dominant chemical adso

254 an empirical model identical in form to the Langmuir-Freundlich equation.

255 The data was analyzed using the Langmuir and Freundlich isotherm models.

256 d anti-BSA antibodies and analyzed using the Langmuir binding theory for the description of the equil

257 This behavior was modeled using the Langmuir isotherm.

258 e study targeted mutants of Rsn-2, using the Langmuir trough, pendant drop tensiometry, and circular

259 Using the Langmuir-Blodgett (LB) technique, a poly(paraphenyleneet

260 Assembled into a film using the Langmuir-Blodgett method, the AuNP LSPR can be tracked w

261 olydispersity (1.09) were prepared using the Langmuir-Blodgett technique to investigate the effects o

262 opic two-dimensional superlattices using the Langmuir-Blodgett technique.

263 prepared on fused silica supports using the Langmuir-Blodgett/Langmuir-Schaeffer technique, which al

264 creasing temperature was evaluated using the Langmuir-Hinshelwood and Eley-Rideal kinetic models, and

265 carbon nanotubes can be assembled using the Langmuir-Schaefer method.

266 h could be successfully accomplished via the Langmuir-Blodgett film deposition technique.

267 -phosphocholine) bilayers, deposited via the Langmuir-Blodgett/Langmuir Schaefer methodology, was inv

268 bic experiment led to data agreeing with the Langmuir isotherm.

269 sures up to 100 kPa, and correlated with the Langmuir model.

270 nformation of Nef was probed upon binding to Langmuir monolayers through the interaction of an N-term

271 Transition from cooperative to Langmuir adhesion in sfGFP-Car9 variants occurs in conce

272 de 1070-cm(-1) band and the trend was fit to Langmuir adsorption kinetics.

273 Modulational instability leads to Langmuir collapse and electron heating that fills in cav

274 surable changes in output current that trace Langmuir isotherms within error of those seen in solutio

275 Langmuir relation (individually transformed Langmuir analysis).

276 est modeled with the bi-Langmuir and the tri-Langmuir isotherm models for Kromasil-C(18) and Discover

277 fugal force, can efficiently excite unstable Langmuir waves in the electron-positron (hereafter e(+/-

278 PIP 2 in a simplified planar system, we used Langmuir monolayers to study the effects of subphase con

279 lly sequenced sheet-forming peptide by using Langmuir techniques, Brewster angle microscopy, attenuat

280 n of a fully asymmetric model envelope using Langmuir-Blodgett and Langmuir-Schaefer methods is now r

281 stems, which were built layer by layer using Langmuir-Blodgett/Schaefer film depositions, included a

282 ed plasma membrane domain organization using Langmuir monolayers of ternary POPC/SM/Chol as well as D

283 absence and presence of phospholipids using Langmuir films, polarization modulated-infrared reflecti

284 e examined by surface X-ray scattering using Langmuir monolayers of dipalmitoylphosphatidylcholine an

285 deposited on gold-coated glass slides using Langmuir-Schaefer films retain functional receptors capa

286 haracterized using UV-Vis spectrometry using Langmuir isotherm formulation and Isothermal Titration M

287 this chemistry with in situ techniques using Langmuir-trough methods and infrared reflection absorpti

288 semiconductor field effect transistor) using Langmuir-Blodgett techniques.

289 face and transferred to silicon wafers using Langmuir-Schaefer deposition.

290 ing with multilayer arachidic acid films via Langmuir-Blodgett deposition results in red-shifting of

291 The deposition is performed via Langmuir-Blodgett (LB) technique.

292 s were deposited onto gold coated slides via Langmuir-Schaefer film deposition and interactions betwe

293 explain the sorption phenomenon out of which Langmuir, Dubinin-Radushkevich, Scatchard and Temkin mod

294 Combined with the Bragg-Williams/Langmuir model and taking into account the experimental

295 With Langmuir monolayers, the lipid packing density can be re

296 t 20 degrees C (median 51 cm(3) g(-1)), with Langmuir affinities (b) of 2-5 atm(-1) (median 3.4 atm(-

297 ic stages, none of which are consistent with Langmuir kinetics.

298 Desiccants can be designed with Langmuir specific surface area >1500 m(2)/g and Langmuir

299 the linear regression of curve-fitting with Langmuir isotherm equation may lead to an incorrect info

300 bundles that are vectorially oriented within Langmuir monolayers at the air-water interface.