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 film properties, UV-vis spectroscopy, epifluore

6 Langmuir isotherms provided better fits to equilibrium d

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

8 Langmuir monolayers (monolayers of insoluble molecules f

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

10 Langmuir-based kinetics, which describe alkanethiolate a

11 Langmuir-Blodgett and Langmuir-Schaeffer deposition and

12 Langmuir-Blodgett films of metallosurfactants were used

13 Langmuir-Schaefer film deposition was used to deposit na

14 Langmuir-Wilhelmy surface balance, fluorescence microsco

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

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

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

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

19 A Langmuir constant of (9.21 +/- 0.71) x 10(3) is determin

20 A Langmuir isotherm model was applied to determine the bin

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

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

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

24 The bilayer was deposited as a Langmuir-Blodgett structure of arachidic (eicosanoic) fa

25 Assuming a Langmuir adsorption isotherm, the dissociation constant

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

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

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

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

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

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

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

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

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

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

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

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

38 (Tempo) to the air/water interface follows a Langmuir isotherm.

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

40 rate of change of surface pressure, pi, in a Langmuir trough following the deposition of surfactant s

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

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

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

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

45 They were best modeled by the sum of a Langmuir and a BET isotherm models.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

60 (18:1, 24:1) have been characterized using a Langmuir-type film balance.

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

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

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

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

65 phospholipase A(2) (cPLA(2)alpha-C2) with a Langmuir monolayer of 1-stearoyl-2-oleoyl-sn-glycero-3-p

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

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

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

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

70 ng calorimetry, fluorescence anisotropy, and Langmuir-Blodgett films suggest that the decreased perme

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 ed concepts of Michaelis-Menten kinetics and Langmuir binding isotherms are combined with fundamental

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

80 ations described by the Michaelis-Menten and Langmuir equations.

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

82 spin-coated thin films, solid solutions, and Langmuir films.

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

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

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

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

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

88 f monolayer and multilayer barium arachidate Langmuir-Blodgett (LB) films is investigated.

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

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

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

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

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

94 r, the adsorption data of caffeine follow bi-Langmuir isotherm model behavior on both adsorbents.

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

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

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

98 1.43 x 10(5) s(-1)) than that of bimolecular Langmuir-Hinshelwood (L-H) pathway (4.29 s(-1)).

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

100 Bs were prepared using the Langmuir-Blodgett/Langmuir-Schaefer method by placing a perdeuterated lipi

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

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

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

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

105 engths in the two leaflets, were prepared by Langmuir-Blodgett deposition and transferred at differen

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

107 Lipid monolayers can be transferred by Langmuir-Schafer deposition onto either silanized glass

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

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

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

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

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

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

114 of the charged species are more conventional Langmuir isotherms.

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

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

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

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

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

120 (3.0 +/- 0.5) x 107 M-1 using an equilibrium Langmuir model.

121 tion onto either silanized glass or existing Langmuir-Blodgett supported monolayers.

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

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

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 mmon case of a convex upward isotherm (e.g., Langmuir), a linear gradient will become curved upward,

127 with a simple convex-upward isotherm (e.g., Langmuir).

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

129 e' term in the LES code in order to generate Langmuir circulations.

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

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

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

133 ation to yield baseline binding information (Langmuir isotherms and affinity constants).

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

135 pectrometry (MS) measurement that integrates Langmuir monolayers.

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

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

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

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

140 A linearized Langmuir adsorption isotherm was used to obtain informat

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

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

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

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

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

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

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

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

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

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

151 ver, at thermodynamic equilibrium a modified Langmuir isotherm governs the bound amount of both speci

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

173 model, run with and without the presence of Langmuir circulations, are presented in order to investi

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

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

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

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

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

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

180 0 was 24.2, 18.8, and 15.1 mg g(-1) based on Langmuir isotherm.

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

182 rediction that is verified by experiments on Langmuir-Blodgett monolayers of amphiphilic [2]rotaxanes

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

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

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

186 d can be readily assembled into close-packed Langmuir-Blodgett films potentially useful for future hi

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

188 s a lipophilic region suitable for promoting Langmuir-Blodgett monolayer formation.

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

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

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

192 -Trp(OPfp) that are best modeled by a simple Langmuir isotherm.

193 to linear peptide epitopes followed a simple Langmuir model.

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

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

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

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

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

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 New Jersey suggest that Langmuir supercells, Langmuir circulations that achieve vertical scales equal

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

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

206 ter off the coast of New Jersey suggest that Langmuir supercells, Langmuir circulations that achieve

207 The Langmuir isotherm describes the adsorption data well and

208 The Langmuir term represents the adsorption of the analyte o

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

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

211 The Langmuir-Hinshelwood model fits the photocatalytic inact

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

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

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

215 ly analyze selection results by applying the Langmuir equation to the binding data to estimate affini

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

242 manner that satisfies the assumptions of the Langmuir model.

243 the fluorescence quenching properties of the Langmuir monolayers were found to be transferred to the

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

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

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

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 However, it uses the Langmuir equation as the local isotherm.

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

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

255 This behavior was modeled using the Langmuir isotherm.

256 oliter plugs could be described by using the Langmuir model and tensiometry results for microliter dr

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

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

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

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

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

262 Asymmetric PSLBs were prepared using the Langmuir-Blodgett/Langmuir-Schaefer method by placing a

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

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

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

274 Langmuir relation (individually transformed Langmuir analysis).

275 etics of Cl- adsorption followed a transient Langmuir adsorption model and allowed measured surface c

276 s of FA data are best accounted for by a tri-Langmuir isotherm model, except for the data of Fmoc-L-T

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

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

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

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

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

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

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

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

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

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

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

299 t the enhanced mixing rates associated with 'Langmuir turbulence' play a significant role in regulati

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