ライフサイエンスコーパス: electrical double layer

1 quantity that dictates the structure of the electrical double layer.

2 teraction and IS reduction that expanded the electrical double layer.

3 arising from a charge imbalance at an inner electrical double-layer, acting across the membrane and

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

5 approach accounts for the key effects of the electrical double layer and spans the electronically adi

6 e identity, charged interface created by the electrical double layer, and supramolecular superstructu

7 sensor results in an enhanced overlapping of electrical double layers, and apparently a more ordered

8 egrating models to reduce the effects of the electrical double layer are subsequently covered.

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

10 of the large current due to charging of the electrical double layer as well as surface faradaic reac

11 mall nanocapillary diameters, the overlap of electrical double layers associated with opposite walls

12 ermittivity of membranes and any cell walls, electrical double layers associated with surface charges

13 Capacitive charging of the electrical double layer at opposing ends of each BPE all

14 faces by changing the characteristics of the electrical double layer at the solid-solution interface,

15 nanotubes to charge the solution side of the electrical double layer at the tube walls.

16 Ionic redistribution within the electrical double layer by fluid flow has been considere

17 Our result suggests that the electrical double layer can be used to pattern nanoscale

18 uantum capacitance of RGO (Cq) and effective electrical double layer capacitance (C(EDL)) contribute

19 ce-potential difference can be determined by electrical double layer capacitance (EDLC) between the n

20 instance, two peaks in the DRTs justify the electrical double layer capacitance and ion diffusion ph

21 he origin of this behaviour by measuring the electrical double-layer capacitance in one to five-layer

22 new theoretical models in understanding the electrical double-layer capacitance of carbon electrodes

23 Experimental electrical double-layer capacitances of porous carbon el

24 Such conversion gives these ACTs an ideal electrical double-layer capacitive behavior.

25 le fast electron/ion transport comparable to electrical-double-layer-capacitive carbons.

26 When integrated with a carbon-based electrical double layer capacitor, nearly ideal electrod

27 e power density and charge-discharge time of electrical double layer capacitors are largely determine

28 h specific energy and high specific power in electrical double layer capacitors.

29 them to surpass the capacity limitations of electrical double-layer capacitors and the mass transfer

30 rge surface areas are typically employed for electrical double-layer capacitors to improve gravimetri

31 e practical energy densities of carbon-based electrical double-layer capacitors.

32 The energy is stored in an electrical double layer composed of an extended Stern la

33 d significant effects on GO stability due to electrical double layer compression, similar to other co

34 ase in electrolyte concentration resulted in electrical double-layer compression of the negatively ch

35 ase in electrolyte concentration resulted in electrical double-layer compression of the negatively ch

36 ations due to intricate ion interactions and electrical double-layer compression.

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

38 llowing us to tune the attractive overlap of electrical double layers, directing particles to dispers

39 n, this sonochemical byproduct collapses the electrical double layer, disrupting the dispersion stabi

40 tion, and we found that the thickness of the electrical double layer does not depend on the charge of

41 lows precise control over the overlap of the electrical double layer (EDL) along the axial direction,

42 The electrical double layer (EDL) at metal oxide-electrolyte

43 ation repulsion and osmotic phenomena in the electrical double layer (EDL) at the clay-water interfac

44 inua, including a continuum representing the electrical double layer (EDL) developed along negatively

45 The classical theory of the electrical double layer (EDL) does not consider the effe

46 ing processes with a direct influence on the electrical double layer (EDL) formation, some of which c

47 The nanoscale electrical double layer (EDL) governs macroscopic phenom

48 by periodic charging and discharging of the electrical double layer (EDL) inhibits both heterogeneou

49 he interface can be further explained by the electrical double layer (EDL) model dominated by the dif

50 Classical electrical double layer (EDL) models are foundational to

51 iver clean water while storing energy in the electrical double layer (EDL) near a charged surface in

52 In aqueous solutions, an electrical double layer (EDL) of Cl(-) and Fe(III) speci

53 ined by the local capacitive response of the electrical double layer (EDL) of the working electrode.

54 The electrical double layer (EDL) plays a central role in el

55 This reduced screening enhances the electrical double layer (EDL) potential magnitude and st

56 transfer and obstructs mass transport in the electrical double layer (EDL) region.

57 utilizing the supercapacitive nature of the electrical double layer (EDL) that occurs at the electro

58 ng entrapped NH(4)(+) ions and enhancing the electrical double layer (EDL) thickness, offering a time

59 lutes were used in the feed solution and the electrical double layer (EDL) was thick.

60 y, that tetraalkylammonium ions populate the electrical double layer (EDL), creating a microenvironme

61 This interface, known as the electrical double layer (EDL), has a different structure

62 ess from the entry of the reactants into the electrical double layer (EDL), to the PCET reaction asso

63 An electrical double layer (EDL)-gated field-effect transis

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

65 s that are comparable to the thickness of an electrical double layer (EDL).

66 Thick electrical double layers (EDLs) (kappa a approximately 1

67 When the electrical double layers (EDLs) formed adjacent to the D

68 tries to assess the influence of overlapping electrical double layers (EDLs) in generating specific e

69 In electrochemical systems, the structure of electrical double layers (EDLs) near electrode surfaces

70 within nanometer-scale channels with finite electrical double layers (EDLs).

71 ch as Ag, with the enhancement attributed to electrical double layer effects and trending with the si

72 However, for kappah < 10, the electrical double layer extends into the nanochannels, a

73 The shielding of the electrical double layer favored ARA-CR hydrophilic inter

74 tudy provides evidence for a sharply defined electrical double layer for large coupling strengths in

75 By dynamically managing the asymmetric electrical double layer formation between the dielectric

76 gration by dynamically regulating asymmetric electrical double layer formation.

77 ned polarization of CF interface dipoles and electrical-double-layer formation.

78 at these interfaces is the structure of the electrical double layer formed when anions or cations co

79 tions have begun to clarify the structure of electrical double layers formed on hydrated clay mineral

80 e capacitance modulations arising within the electrical double layer from the RTIL- CO(2) interaction

81 nt and charge modulations arising within the electrical double layer from the RTIL-NO interactions th

82 or the detection of cardiac troponin I using electrical double layer gated high field AlGaN/GaN HEMT

83 erface are directly detected using sub-10-nm electrical double layer-gated silicon nanowire field-eff

84 atic programmable-flow system to disrupt the electrical double layer generated at the DP/organic phas

85 surfaces influenced by the properties of the electrical double layer in the aqueous phase film and su

86 n particular to those solutions producing an electrical double layer in the order of a few tens of na

87 phenomenon, a molecular-level picture of the electrical double layer in working devices is still lack

88 al positioning of organic cations within the electrical double layer independently affect reactivity.

89 However, the structure of the electrical double layer influences the concentration of

90 t of particle retention is not controlled by electrical double layer interactions.

91 ible for such shifts: 1) the formation of an electrical double layer (ionic mechanism), and 2) change

92 The characterization of electrical double layers is important since the interfac

93 lar electrochemistry, provide benchmarks for electrical double layer models, and serve as a diagnosti

94 It is based on a fundamental aspect of electrical double layers, namely, their huge capacitance

95 w is insufficient to accurately describe the electrical double layer of aqueous interfaces.

96 osition of redox-active moieties, within the electrical double layer, on the apparent formal potentia

97 tion and diffusion restriction, thus forming electrical double layers over the leaf surface and showi

98 he ion exclusion-enrichment effect caused by electrical double layer overlapping induces cationic sel

99 a new protocol for QD film deposition using electrical double-layered PbS QD inks, prepared by solut

100 One aim is to yield insight into electrical double layer physics and study the applicabil

101 The nanoscale electrical double layer plays a crucial role in macrosco

102 s well as the charge at the cell surface (an electrical double layer) producing an extracellular elec

103 of zero charge is generally consistent with electrical double layer properties, but the irregular pa

104 to capacitive coupling between V(m) and the electrical double layer, rather than molecular transport

105 efficacy remains constrained by interfacial electrical double-layer screening in aqueous solutions.

106 el instrument, the Scanning Electrometer for Electrical Double-layer (SEED) has been developed to mea

107 e method is called Scanning Electrometer for Electrical Double-layer (SEED).

108 capacitance is governed by classical surface electrical double layers, showing no evidence of quantum

109 The electrical double layer significantly responds to the ap

110 tation of the water molecules as well as the electrical double layer strength increased further when

111 lar dynamics simulations, we investigate the electrical double-layer structure occurring at the inter

112 potential of the carbon layer determines the electrical double-layer structure that, in turn, affects

113 havior can be further tuned by modifying the electrical double layers surrounding the nanoparticles.

114 he liquid crystal and the diffuse part of an electrical double layer that evolves upon oxidation of f

115 of charges suspended in the medium and to an electrical double layer that forms at each electrode-med

116 el with a mean pore size on the order of the electrical double layer thickness imparts ion-permselect

117 rged protein at distances beyond that of the electrical double-layer thickness.

118 he potential drop from the initiation of the electrical double layer to different distances above it.

119 interphase starting from a few 0.1 nm thick electrical double layer to the full three-dimensional na

120 Electrical double layer transistors using ionic liquids

121 of buffer electrolyte, the thickness of the electrical double layer was extended so the interfacial

122 ch allowed us to obtain the thickness of the electrical double layer when multivalent inorganic catio

123 ter molecules within the diffuse part of the electrical double layer, which are ordered by the surfac

124 mulation of hydronium ions, H(3)O(+), in the electrical double layer, which drive the reaction togeth