ライフサイエンスコーパス: double layer

1 on-coupled electron transfer in the electric double layer.

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

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

4 decrease in the capacitance of the electric double layer.

5 nd IS reduction that expanded the electrical double layer.

6 the reaction mechanism and structure of the double layer.

7 of LiF due to the presence of anions in the double layer.

8 hat dictates the structure of the electrical double layer.

9 when the molecules were within the electric double layer.

10 explicitly considering the charged electric double layer.

11 inner and outer part of the electrochemical double layer.

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

13 , hydration energy, and overlapping electric double layers.

14 to couplings of electric fields and electric double layers.

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

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

17 duced graphene oxide-fullerene composite and double layered acrylamide functionalised reduced graphen

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

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

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

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

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

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

24 We then define a limit of thin electrical double layer and illustrate the emergence of the charact

25 counts for the key effects of the electrical double layer and spans the electronically adiabatic and

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

27 citon condensation in two-dimensional atomic double layers and opens up opportunities for exploring c

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

29 re carried out, which provide information on double-layer and van-der-Waals forces at the interface.

30 charged interface created by the electrical double layer, and supramolecular superstructure all affe

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

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

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

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

38 otential across the adsorbed polyelectrolyte double layer at the confining surface is found to decrea

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

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

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

42 able to quantify the amount of charge in the double layers at the solution/electrode interface for di

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

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

45 ectrode/electrolyte system when the electric double layer between the nanorods does not overlap.

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

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

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

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

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

55 The monitored drift in R(CT) and double layer capacitance during the conditioning suggest

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

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

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

59 c terms (uncompensated resistance, R(u), and double layer capacitance, C(dl)).

60 sistance, R (and solution conductivity), and double layer capacitance, C, can be extracted from this

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

62 g different methods (namely, the ball model, double layer capacitance, isotope exchange, and redox pe

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

64 (R(s)), charge-transfer resistance (R(ct)), double-layer capacitance (C(dl)), and Warburg impedance

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

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

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

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

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

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

71 etween the passive tissue properties and the double-layer capacitance of electrodes.

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

73 are discovered with a remarkable nonfaradaic double-layer capacitance that exists due to the consider

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

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

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

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

78 Furthermore, these transistors with double-layer capacitive dielectric can mimic the synapti

79 ctron/ion transport comparable to electrical-double-layer-capacitive carbons.

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

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

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

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

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

85 a great deal of research on electrochemical double layer capacitors (EDLCs).

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

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

88 The electrochemical double-layer capacitors (EDLCs) are highly demanded elec

89 rpass the capacity limitations of electrical double-layer capacitors and the mass transfer limitation

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

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

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

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

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

95 s is essential to control the performance of double-layer capacitors.

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

97 nance imaging experiments of electrochemical double-layer capacitors.

98 The double-layer capacity and alternating current measuremen

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

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

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

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

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

104 (e-COFs) that are able to perform excellent double-layer charge storage is reported.

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

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

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

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

109 trolyte concentration resulted in electrical double-layer compression of the negatively charged 2D NM

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

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

112 Rp VP1 in both the triple-layered virion and double-layered core, as determined by cryo-electron micr

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

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

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

116 to tune the attractive overlap of electrical double layers, directing particles to disperse, crystall

117 disconnections, where both single-layer and double-layer disconnections have important contributions

118 cture and ultrafast dynamics of the electric double layer (EDL) are central to chemical reactivity an

119 olid interfacial interactions at an electric double layer (EDL) are studied in various research field

120 nderstanding of the formation of an electric double layer (EDL) at a liquid-solid interface in physic

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 ified sensitivity of solution-gated electric double layer (EDL) HEMT-based biosensors, which demonstr

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

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

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

127 In aqueous solutions, an electrical double layer (EDL) of Cl(-) and Fe(III) species at 0.5 m

128 local capacitive response of the electrical double layer (EDL) of the working electrode.

129 the supercapacitive nature of the electrical double layer (EDL) that occurs at the electrolytic-elect

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

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

132 related to the overlap of the electrostatic double layers (EDL) surrounding the NPs and the agarose

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

134 cules at fixed positions within the electric double layer, EDL, has been determined experimentally.

135 Electric double layers (EDLs) formed in electrolyte-gated field-e

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

137 through the cell by storing ions in electric double layers (EDLs) within charged micropores.

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

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

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

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

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

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

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

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

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

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

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

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

150 explore diversified applications of electric double layer FETs (EDL-FETs), a triboiontronic transisto

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

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

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 orous carbon-based electrodes, including the double layer formation in confined nanopores.

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

159 s (during the initial charging), an electric double layer forms at the electrode/electrolyte interfac

160 ce modulations arising within the electrical double layer from the RTIL- CO(2) interactions through A

161 This is the first time that active double-layered furcellaran/gelatin hydrolysate films con

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

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

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

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

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

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

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

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

170 d developed across the molecular-scale ionic double layer (IDL) when the junction is placed under rev

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

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

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

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

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

176 er and demonstrate the formation of electric double-layer in liquid-solid CE.

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

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 ch shifts: 1) the formation of an electrical double layer (ionic mechanism), and 2) changes in the el

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

182 The formation of the double layer is directed by Li(+) and the electrode surf

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

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

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 on single layer materials but different from double layer materials.

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

189 e), entrapped into chitosan-calcium alginate double layer microcapsules, for the production of a Pale

190 dure, applying the chitosan-calcium alginate double layer microcapsules, for the production of Riesli

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

196 aled breath samples were collected using 2-L double-layered Nalophan bags, and were analyzed using se

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

198 ed at variable distances within the electric double layer of a transparent conductive oxide as a func

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

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

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

202 and Gram-negative bacteria are encased in a double layer of membranes.

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

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

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

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

207 clarifying the structure and dynamics of the double layer, of adsorbed species on electrode surfaces,

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

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

210 In this paper, electric double layer p-i-n junctions in WSe(2) are shown with su

211 n top of host cells, but it is embraced by a double-layer parasitophorous vacuole membrane derived fr

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

213 ol of an intact, inner capsid particle (the "double-layer particle," or DLP).

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

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

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

217 d RNA [+RNA] synthesis) by VP1 occurs within double-layered particles (DLPs), while genome replicatio

218 study frozen-hydrated specimens of rotavirus double-layered particles and HIV-1 virus-like particles

219 virions was significantly prevented and only double-layered particles were detected.

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

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

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

223 ion and doping effects through demonstrating double-layered PEA(2)PbI(4)/PEA(2)SnI(4) heterostructure

224 For many years, double-layer phospholipid membrane vesicles, released by

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

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

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

228 s self-assembled glutaraldehyde-cross-linked double-layered polyethylenimine (PEI-GA-PEI)-modified na

229 Therefore, a double-layer polymer electrolyte is investigated, in whi

230 The structure of this double layer predicts the eventual interphasial chemistr

231 ts should thermodynamically decompose in the double layer prior to the Mg(2+)/Mg(0) reduction, leadin

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

233 We also find that all of the important double-layer properties, such as charge amplification, e

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

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

236 Both electrolytes are highly reactive in the double layer region where the solvated species have no d

237 presence of OH(ad)-(H(2)O) (x)-AM(+) in the double-layer region facilitates the OH(ad) removal into

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

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

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

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

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

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

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

245 tions between type 1 MNV and presence of the double-layer sign (P < 0.001).

246 findings included choroidal elevation and a double-layer sign (separation of hyperreflective retinal

247 Reduction in the double-layer sign became evident as the lesions began to

248 They detected a double-layer sign in 24 of 33 eyes with subclinical MNV

249 The senior grader detected a double-layer sign in 29 of 33 eyes with subclinical MNV

250 es with subclinical MNV and did not detect a double-layer sign in 56 of 67 eyes without MNV.

251 es with subclinical MNV and did not detect a double-layer sign in 58 of 67 eyes without MNV, achievin

252 tion was found between the resolution of the double-layer sign on SD OCT and FAF findings.

253 The double-layer sign on SD OCT may be a useful finding in m

254 Presence of the double-layer sign on structural OCT B-scans was associat

255 e of a double-layer sign to determine if the double-layer sign predicted subclinical macular neovascu

256 tion (AMD) were graded for the presence of a double-layer sign to determine if the double-layer sign

257 The presence of a double-layer sign was used as a predictive sign for subc

258 nd increased choroidal elevation on OCT, the double-layer sign was very prominent.

259 flectivity as characteristic features of the double-layer sign when NE-MNV was present.

260 -source (SS) OCT angiography (OCTA) and the "double-layer sign" on structural spectral-domain OCT (SD

261 The electrical double layer significantly responds to the applied poten

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

263 ects, the electrostatic energy stored in the double-layer structure is enhanced with an increase in t

264 dielectric mismatch remarkably influence the double-layer structure of a polyelectrolyte solution con

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

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

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

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

269 A diffuse double layer surface complexation model was developed fo

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

271 be further tuned by modifying the electrical double layers surrounding the nanoparticles.

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

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

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

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

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

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

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

279 A yielded higher amplitude signals, when the double layer thickness is comparable to the wavelength o

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

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

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

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

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

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

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

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

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

289 Electrical double layer transistors using ionic liquids as the gate

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

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

296 he space-charge distribution in the electric double layer, which blocks the long-range migration of C

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

298 stomers of opposite polarity yields an ionic double layer, which is capable of rectifying and switchi

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

300 interlayer excitons in MoSe(2)-WSe(2) atomic double layers with a density of up to 10(12) excitons pe