ライフサイエンスコーパス: double layer

1 decrease in the capacitance of the electric double layer.

2 nd IS reduction that expanded the electrical double layer.

3 the reaction mechanism and structure of the double layer.

4 formation and rearrangement of the electric double layer.

5 o screen the electric field generated at the double layer.

6 between surface-bound water and that in the double layer.

7 h both the electrode surface and the diffuse double layer.

8 ometry of nanopore, and the thickness of the double layer.

9 , hydration energy, and overlapping electric double layers.

10 to couplings of electric fields and electric double layers.

11 ion caused irreversible stacking, leading to double layers.

12 covered by any coating as thick as graphene double layers.

13 s are single layered; cytoplasmic arrays are double layered.

14 the other was a flattened tube and therefore double-layered.

15 he higher concentration of Cu(2+) within the double layer above the membrane was largely responsible

16 s concentration of a cationic dye within the double layer adjacent to an anionic phospholipid monolay

17 Starting from the double layer adsorption model, we determined (in additio

18 se, fructose, glucose and maltitol), using a double layer adsorption model.

19 trengths, the incomplete overlap of electric double layer allows more facile ionic transfer across th

20 The use of a double layer allows more protection for the explant with

21 This ligand double layer and a high ligand density (3.6 DDT molecule

22 values but also on the shape of the electric double layer and analyte ion valence.

23 The model is based on a theory of the thin double layer and corresponding expressions used for the

24 mber selective cleavage, from a monolayer to double layer and up to 23 atomic layers.

25 Shot within the follicle epithelium leads to double layering and accumulation of actin and ZO-1 in be

26 d the anatomic framework encapsulated by the double-layer and triple-layer signs.

27 ers with different organizations (single and double layers) and morphologies (linear-like and annular

28 lts in an enhanced overlapping of electrical double layers, and apparently a more ordered "ice-like"

29 red to the smooth channel even for very thin double layers, and hence plays an important role in micr

30 dels to reduce the effects of the electrical double layer are subsequently covered.

31 surface structure and charge of the electric double layer around a nanodroplet and its structural cha

32 Such adsorption creates an electrical double layer around the CNTs within which the concentrat

33 rents caused by an increased electrochemical double layer as well as enhanced catalytic currents due

34 ge current due to charging of the electrical double layer as well as surface faradaic reactions.

35 fford countless features that are single and double layers as judged by their AFM heights of hAFM app

36 pillary diameters, the overlap of electrical double layers associated with opposite walls of the nano

37 and represents the effective electrochemical double layer at a gas-solid interface.

38 Capacitive charging of the electrical double layer at opposing ends of each BPE allows an AC e

39 ssociated with the formation of the electric double layer at the droplet-surface interface.

40 the capacitative response of the channel and double layer at the electrode surfaces.

41 ization of electrolyte ions into an electric double layer at the surface of each porous electrode.

42 harge sensitivity arises because the diffuse double layers at the nanopipette and the surface interac

43 ntraction and genome release of phages with "double-layered" baseplates were unknown.

44 in solution indicate that they consist of a double-layered beta-sheets where each monomer folds into

45 e binding energy and the interactions in the double layer between hydroxide-oxides and H---OH are fou

46 n the surface of Sr3(Ru1-xMnx)2O7, which has double-layer building blocks formed by (Ru/Mn)O6 octahed

47 leads to the loss of the first RP rock-salt double layer, but growing with a strontium-rich surface

48 by surface modification due to thin electric double layers, but the morphology changes dramatically a

49 Ionic redistribution within the electrical double layer by fluid flow has been considered to be the

50 Our result suggests that the electrical double layer can be used to pattern nanoscale features.

51 citance of RGO (Cq) and effective electrical double layer capacitance (C(EDL)) contribute significant

52 (alpha), uncompensated resistance (Ru), and double layer capacitance (CDL) can be reported using the

53 l difference can be determined by electrical double layer capacitance (EDLC) between the nano-gap ele

54 periodic component are essentially devoid of double layer capacitance contributions allowing the fara

55 ic components contain contributions from the double layer capacitance current, thereby allowing detai

56 yte to separate the effects of nanocapillary double layer capacitance from those of nanocapillary geo

57 Because of the large double layer capacitance of CIM carbon, CIM carbon-based

58 resistance at the electrode tip x electrode double layer capacitance), which is a function of the ti

59 nt), Ru (uncompensated resistance), and Cdl (double layer capacitance).

60 second harmonics that contain details of the double layer capacitance, and Faradaic ac higher order h

61 quently performed electrochemical impedance, double layer capacitance, cyclic voltammetry, and galvan

62 ated method requires a perfect model for the double layer capacitance.

63 attribute this discrepancy to the effects of double-layer capacitance charging and adsorbed species i

64 Here, we describe the significance of the double-layer capacitance effect in polar rubbery dielect

65 s, we attribute the above observation to the double-layer capacitance effect, even though the ionic c

66 ifferent from previously reported OFETs with double-layer capacitance effects, our devices showed unp

67 sizes from 0.6 to 2.25 nanometer and studied double-layer capacitance in an organic electrolyte.

68 f this behaviour by measuring the electrical double-layer capacitance in one to five-layer graphene.

69 tical models in understanding the electrical double-layer capacitance of carbon electrodes, and on op

70 ce coverage, charge-transfer resistance, and double-layer capacitance of the interface using a simple

71 they offer high surface areas for increased double-layer capacitance, open structures for rapid ion

72 DOT(PTS), due to the formation of additional double-layer capacitance.

73 Experimental electrical double-layer capacitances of porous carbon electrodes fa

74 version gives these ACTs an ideal electrical double-layer capacitive behavior.

75 the electrolyte between two electrodes and a double layer capacitor, an electron-transfer resistor, a

76 en integrated with a carbon-based electrical double layer capacitor, nearly ideal electrode propertie

77 The electric characteristics of electric-double layer capacitors (EDLCs) are determined by their

78 Electrochemical double layer capacitors (EDLCs) employing ionic liquid e

79 ility relative to batteries, electrochemical double layer capacitors (EDLCs) have emerged as an impor

80 Electrochemical double layer capacitors (EDLCs), or supercapacitors, rel

81 sity and charge-discharge time of electrical double layer capacitors are largely determined by how fa

82 -high volumetric performance electrochemical double layer capacitors based on high density aligned na

83 energy and high specific power in electrical double layer capacitors.

84 Electric double-layer capacitors (DLCs) can have high storage cap

85 Research in electric double-layer capacitors (EDLCs) and rechargeable batteri

86 d here are the first simulations of electric double-layer capacitors based on carbon nanotube forests

87 Electrochemical double-layer capacitors exhibit high power and long cycl

88 areas are typically employed for electrical double-layer capacitors to improve gravimetric energy st

89 t with experimental capacitances of electric double-layer capacitors utilizing carbon nanotube forest

90 Supercapacitors (or electric double-layer capacitors) are high-power energy storage d

91 n the development and use of electrochemical double-layer capacitors, fuelled by the availability of

92 n comparison to aqueous and organic electric double-layer capacitors, this system enhances energy by

93 energy densities of carbon-based electrical double-layer capacitors.

94 nance imaging experiments of electrochemical double-layer capacitors.

95 The electrode double layer capacity is not appreciably diminished by t

96 The double-layer capacity and alternating current measuremen

97 TG recognition signal into the change of the double-layer capacity dependence on the 6TG concentratio

98 Our months-long studies indicate that a double layer capping of Al2O3 and hydrophobic fluoropoly

99 dition, we determine how the electrochemical double layer changes as a function of both the electroly

100 up to a factor of 63 as the magnitude of the double layer charge density was increased.

101 ia independent pseudocapacitive and electric double layer charge storage channels.

102 The absence of double layer charging current in cyclic voltammograms of

103 225 core nanoparticle that display quantized double layer charging voltammetry consistent with a Au22

104 They are too slow to be explained by double layer charging, and chronoamperometry data showed

105 ral details of eluted peaks and of quantized double-layer charging features in the differential pulse

106 Our method utilizes double-layer colloidal crystal templates in conjunction

107 cant changes in the magnitude of the compact double layer component (C(COMPACT), equivalent to the St

108 caused, primarily, by changes in the diffuse double layer component (C(DIFFUSE)) of C(MPC).

109 The energy is stored in an electrical double layer composed of an extended Stern layer, which

110 Optical absorption experiments show that all double-layer compounds exhibit a blue shift in their abs

111 nt effects on GO stability due to electrical double layer compression, similar to other colloidal par

112 trolyte concentration resulted in electrical double-layer compression of the negatively charged fulle

113 acteriophages from the family Myoviridae use double-layered contractile tails to infect bacteria.

114 Stagg et al. have now visualized the double-layered COPII coat using electron cryomicroscopy,

115 and self-assembles with high fidelity into a double-layered cross-beta structure.

116 some carboxy-terminally cleaved AQP0, forms double-layered crystals that recapitulate in vivo juncti

117 ted by probing the properties of the diffuse double layer (DDL) at the cellular interface, and the te

118 The molecular structure of the electrical double layer determines the chemistry in all electrochem

119 ochemical byproduct collapses the electrical double layer, disrupting the dispersion stability and lo

120 e found that the thickness of the electrical double layer does not depend on the charge of anions.

121 howed higher H(+) mobility, and the electric double layer (EDL) capacitance increased to 145 F g(-1)

122 amined, and it has been proven that electric double layer (EDL) formed on porous electrode surfaces a

123 expansion depends on the extent the electric double layer (EDL) is altered in a low salt concentratio

124 e can be further explained by the electrical double layer (EDL) model dominated by the diffuse layer.

125 water while storing energy in the electrical double layer (EDL) near a charged surface in a capacitiv

126 that modulates the charge in the electrical double layer (EDL).

127 comparable to the thickness of an electrical double layer (EDL).

128 he importance of chemical doping in electric double-layer (EDL) gating experiments with superconducti

129 Thick electrical double layers (EDLs) (kappa a approximately 1) exhibit c

130 When the electrical double layers (EDLs) formed adjacent to the DNA nanopart

131 Recently, electric double layers (EDLs) have been regarded as a promising c

132 ometer-scale channels with finite electrical double layers (EDLs).

133 The kinetic data show a small double layer effect when the concentration of HClO4 used

134 culations, which account for electrochemical double-layer effects on the conductance of the NDI junct

135 adsorption, electron transfer kinetics, and double-layer effects on the nanoscale.

136 ce (Cm) regardless of holding voltage due to double-layer effects.

137 by protein-lipid interactions and electrode double-layer effects.

138 In this sandwich architecture, the double-layer electric field at the Li/polymer interface

139 rface of the reduced graphene oxide-graphene double-layer electrode via pi-pi bonds and then hybridiz

140 ved from the reduced graphene oxide-graphene double-layer electrode, a 42% and 36.7% increase, respec

141 Non-cross-linked and cross-linked double-layer emulsions (with and without salt) were then

142 Laccase was added to the double-layer emulsions to covalently crosslink the adsor

143 ew nanometers of an electrode surface (i.e., double layer) engender fluid flow within a serpentine ch

144 ed that exsM mutant spores were encased by a double-layer exosporium, both layers of which were compo

145 obtained through capacitive mixing based on double layer expansion depends on the extent the electri

146 In the modeled system, the electric double layer extends into the channel, and consequently,

147 However, for kappah < 10, the electrical double layer extends into the nanochannels, and due to c

148 Our simulations of the solvent protection of double-layered fibril and globulomer models reproduce ex

149 NA length, demonstrating a dependence on the double layer field.

150 es evidence for a sharply defined electrical double layer for large coupling strengths in contrast to

151 ged bilayers that includes the electrostatic double-layer force of the Derjaguin-Landau-Verwey-Overbe

152 tion, we demonstrate that the AFM can detect double layer forces at a separation of several screening

153 ch other and the pore wall via electrostatic double layer forces.

154 e long-range, exponentially decaying diffuse double-layer forces observed across ionic liquids exhibi

155 ts using the van der Waals and electrostatic double-layer forces of the Derjaguin-Landau-Verwey-Overb

156 ss the electrodes engendered electrochemical double layer formation at the Al(2)O(3)-solution interfa

157 ation of CF interface dipoles and electrical-double-layer formation.

158 ction of cardiac troponin I using electrical double layer gated high field AlGaN/GaN HEMT biosensor.

159 We demonstrate a working concept of a double layer graphene field effect device that utilizes

160 -phase and anti-phase vibrational modes of a double layer graphene nanoribbon is achieved by introduc

161 amondene by performing Raman spectroscopy of double-layer graphene under high pressure.

162 proximately 14 times higher than that of the double-layer graphene.

163 electrodes and ionic solutions (the electric double layer) has been investigated as a source of clean

164 averaged flow-field near a cell in a run has double-layered helical streamlines, with a time-dependen

165 and photodetector design based on a graphene double-layer heterostructure.

166 (MQ) particles as the post-TG product of all double-layer hybrids.

167 e report the novel system of nickel-aluminum double layered hydroxide (NiAl-LDH) nanoplates on carbon

168 ity with lattice spacing similar to those of double-layered hydroxides.

169 s thus viable to obtain energy from electric double layers if these are successively contacted with w

170 fluenced by the properties of the electrical double layer in the aqueous phase film and surface funct

171 r to those solutions producing an electrical double layer in the order of a few tens of nanometers (i

172 a molecular-level picture of the electrical double layer in working devices is still lacking as few

173 MspA is known to form double layers in which it acts as nanoscopic surfactant.

174 he entropy associated with the electrostatic double layer, in agreement with theoretical predictions.

175 NO synthase (iNOS) were also observed in the double-layer infection model, and abrogation of iNOS exp

176 ved to include the effects of the capacitive double layer inside the nanocapillaries as well as the i

177 ce microscope (AFM) is sensitive to electric double layer interactions in electrolyte solutions, but

178 le retention is not controlled by electrical double layer interactions.

179 edox charge storage, commensurate to surface double layer ion exchange at carbon electrodes.

180 se electric double layers, where the diffuse double layer is comprised of effectively dissociated ion

181 Nevertheless, the double layer is distorted at high macroion volume fracti

182 e ferrocene moiety and the initiation of the double layer is increased.

183 When the thickness of the electric double layer is relatively large, the PBM and SVM predic

184 resistance and capacitance variations of the double layer is suggested here.

185 layers, in which the key layer, an electric double layer, is inserted between a top layer, made of A

186 The presence of this double layer leads to reversible, selective uptake and r

187 densities in simple single layer devices and double layer light emitting devices compared to those wi

188 This double-layer location indicates that C2B interacts in a

189 on single layer materials but different from double layer materials.

190 ope (TEM), CLDIs were bounded by an atypical double-layered membrane, approximately 20 nanometers thi

191 sdermal protein delivery using bullet-shaped double-layered microneedle (MN) arrays with water-swella

192 rast, the importance of imperfections in the double layer model is minimized when analysis is perform

193 A theory based upon a double layer model was proposed wherein kosmotropic anio

194 face is well-described with an electrostatic double-layer model for the QD/solvent interface.

195 This is in contrast to a traditional uniform double-layer model where the net current flows along the

196 Cocultures of CaCo-2 cells and DCs in a "double-layer" model followed by infection with OmpA(+) C

197 early demonstrate that, outside of the bound double layer, most of the ions in [C4mim][NTf2] are not

198 are single-layer (n = 1) in 2D-[(MQ)(L)] but double-layer (n = 2) in 2D-[(M2Q2)(L)].

199 based on a fundamental aspect of electrical double layers, namely, their huge capacitance.

200 trate that AD and ADA lamellae are made of a double layer of co-oligomers with overlapping and strong

201 TX3L acted on host and pathogen to achieve a double layer of immunity within a safe reserve in the in

202 arge region around each seed consisting of a double layer of ions, where the integrity of the layer i

203 Bruch membrane and were in proximity to the double layers of flattened RPE detachment.

204 Double layers of Li ions are sandwiched between the stac

205 f 2D nanocrystals with an exact thickness of double layers of molecules is driven by directional crys

206 lectronic junction comprising a single (or a double) layer of alkyl-thiol and alkyl-silane molecules

207 Electroosmosis, originating in the double-layer of a small liquid-filled pore (size R) and

208 Lipid droplets coated by a double-layer of biopolymers (gelatin-pectin) were prepar

209 The interferometric biosensor uses a double-layer of porous Si comprised of a top layer with

210 of this surface leads to the formation of a double-layer of separating membranes between the two dau

211 Double-layered oligomers associating through the C-termi

212 Linear-like and annular-like double-layered oligomers with the NN interface are energ

213 led study of the effect of the surface ionic double layer on electronic passivation of QD surfaces, w

214 redox-active moieties, within the electrical double layer, on the apparent formal potential and on th

215 ation of these individual nanopores suggests double layer overlap is not required to form an ion depl

216 usion-enrichment effect caused by electrical double layer overlapping induces cationic selectivity of

217 yered parallel-stranded beta-sheets and (ii) double-layered parallel-stranded antiparallel beta-sheet

218 VP7, surround a transcriptionally competent, double-layer particle (DLP), which they deliver into the

219 ds, of the rotavirus inner capsid particle ("double-layer particle" or DLP) at a resolution suitable

220 data and experimental data of the rotavirus double-layer particle.

221 ity Abs at the viral RNA release pore in the double-layer particle.

222 The structure of the RV6-25 antibody-double-layered particle (DLP) complex indicated a very c

223 virion is lost during cell entry, yielding a double-layered particle (DLP) that directs synthesis of

224 tavirus inner capsid particle, known as the "double-layered particle" (DLP), is the "payload" deliver

225 an in vitro approach with purified rotavirus double-layer particles, nascent single-stranded RNA (ssR

226 ulfide cross-linked VP7 mutant which recoats double-layered particles (DLPs) as efficiently as does w

227 igh-resolution structure of bovine rotavirus double-layered particles, we predicted these epitopes to

228 o the internal protein VP6 on the surface of double-layered particles, which is normally exposed only

229 ability to block the transcriptional pore on double-layered particles.

230 ocol for QD film deposition using electrical double-layered PbS QD inks, prepared by solution-phase l

231 The presence of pi-shape structure as a double-layer physical barrier allowed detection of AFB1

232 One aim is to yield insight into electrical double layer physics and study the applicability of cont

233 Herein, we report a new class of double-layered plasmonic-magnetic vesicle assembled from

234 The electrochemical double layer plays a critical role in electrochemical pr

235 channels, the electric field inherent to the double layer produces transverse species distributions t

236 we discern the shape of the electrochemical double layer profile.

237 ugh to have, because of overlapping electric double layers, properties similar to those of interlayer

238 A double-layer protofibril structure is also proposed in w

239 As such, the Cu(2+) concentration within the double layer region was greatly amplified relative to it

240 ibution of negative charges in the electrode double-layer region when the aptamer adopts a folded con

241 his to the high entropic repulsion (electric double layer repulsion) due to the large size of molecul

242 ath ionic strength (and hence, electrostatic double-layer repulsion), as well as increasing Ca(2+) co

243 n EFFF through systematic disruptions of the double layer resulting in a stronger effective field in

244 onds with a transient modulation of electric double layers, resulting in an extraordinary sensitivity

245 ter capsid proteins VP4 and VP7 to authentic double-layered rotavirus subviral particles (DLPs) in th

246 By utilizing this double-layer screening method, six positive mutants were

247 nt, the Scanning Electrometer for Electrical Double-layer (SEED) has been developed to measure multip

248 called Scanning Electrometer for Electrical Double-layer (SEED).

249 The complex is organized as a double-layered shallow corkscrew, with the AAA+ and AAA+

250 electrodes) and the formation of an electric double layer shields the channel, making the effective f

251 is governed by classical surface electrical double layers, showing no evidence of quantum contributi

252 The electrical double layer significantly responds to the applied poten

253 situ via electron transport spectroscopy in double-layered Sr(3)(Ru(1-x)Mn(x))(2)O(7) (x = 0 and 0.2

254 ng corresponding modulation of electrostatic double layer, steric hydration, and hydrophobic interact

255 of proton reduction by an alteration of the double-layer structure induced by a saturated surface co

256 f the carbon layer determines the electrical double-layer structure that, in turn, affects the ionic

257 Double-layered structures with a helical morphology will

258 urcation coverage with extensive segments of double-layered struts and inappropriately apposed struts

259 superior to those of commercially available double-layer supercapacitors, pseudocapacitors, lithium-

260 ing a Langmuir isotherm model, and a diffuse double layer surface complexation model (DLM) was develo

261 A diffuse double layer surface complexation model was developed fo

262 edict and subsequently show that such a TiO2 double-layer surface reconstruction enhances the oxygen

263 fast temperature perturbations on a par with double-layer susceptibility.

264 n suture material, suture format, single- vs double-layer sutures, interrupted vs continuous sutures,

265 ration is described in terms of the electric double layer that affects the potential difference drivi

266 air-water interface, generating an electric double layer that facilitates wetting.

267 suspended in the medium and to an electrical double layer that forms at each electrode-medium interfa

268 ectrical organization of the electrochemical double layer, the experimental verification of these mod

269 They include the capacitance of the electric double layer, the resistance of the interfacial charge t

270 Using principles from double-layer theory we derived an approximate linear equ

271 hate buffered saline (DPBS) electrolyte, the double layer thickness can be manipulated so that the in

272 ean pore size on the order of the electrical double layer thickness imparts ion-permselectivity (cati

273 r-scale electrokinetic systems, the electric double layer thickness is comparable to characteristic c

274 along nanoscale channels having an electric double-layer thickness comparable to the channel size.

275 The FB mode is formed within a double layer, thin-film stack where at subwavelength thi

276 l drop from the initiation of the electrical double layer to different distances above it.

277 of the montmorillonite basal plane electric double layer to the montmorillonite edge may screen the

278 ride layers with controlled thicknesses from double layers to bulk.

279 onic conductivity gradients outside electric double layers to produce flow instabilities.

280 may be relevant for applications of electric double layer transistor devices.

281 (x = 0.15) ultrathin films, via the electric double layer transistor technique.

282 pled valley photocurrent, within an electric-double-layer transistor based on WSe2, whose direction a

283 lectrolytes or ionic liquids in the electric double-layer transistor configuration.

284 ties above 10(13) cm(-2) in rubrene electric double layer transistors (EDLTs).

285 Electrical double layer transistors using ionic liquids as the gate

286 Nanoporous graphene- based electric-double-layer transistors (EDLTs) are successfully fabric

287 are one unit cell thick, and fabrication of double-layer transistors.

288 day below-knee cast) compared with that of a double-layer tubular compression bandage in promoting re

289 a proportion of truncated protein, produced double-layered two-dimensional (2D) crystals, which disp

290 0, determined by electron crystallography of double-layered two-dimensional crystals.

291 nature of the flow, the contribution of the double layer under the conditions mentioned above should

292 ity of the surfactant in the electrochemical double layer under the conditions of electrolysis.

293 electrolyte, the thickness of the electrical double layer was extended so the interfacial electric fi

294 cal cell and the capacitance of the electric double-layer, we are able to determine the time-constant

295 Also, areas of stacked double layers were found, and these increased in extent

296 bilayer but is localized within the aqueous double layer when C2B is bound.

297 us to obtain the thickness of the electrical double layer when multivalent inorganic cations are pres

298 n of both bound (Stern) and diffuse electric double layers, where the diffuse double layer is compris

299 The latter is part of a ligand double layer, which consists of dynamically bound dodeca

300 DLVO relates the ionic double layers, which enclose the particles, to their eff