2021
DOI: 10.1039/d1cp01435h
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Evaluation of static differential capacitance at the [C4mim+][TFSA]/electrode interface using molecular dynamics simulation combined with electrochemical surface plasmon resonance measurements

Abstract: Molecular dynamic (MD) simulations have been performed for 1-butyl-3-methylimidazolium bis(trifluoromethanesulfonyl)amide ([C4mim+][TFSA−]), an ionic liquid (IL), on a charged graphene electrode to achieve the quantitative analysis of the static differential capacitance...

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Cited by 14 publications
(19 citation statements)
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“…S2a) [33]. The negative Δθ shift reflects a lower local refractive index for the cation rich ionic layer in the EDL than for the anion rich counterpart, which was revealed by our recent study combining ESPR and molecular dynamics simulation [42]. After the negative shift, Δθ switched to a positive shift at potentials where the cathodic deposition occurs (<−0.7 V).…”
Section: -4 Simulation Of Resonance Angle Shiftmentioning
confidence: 78%
“…S2a) [33]. The negative Δθ shift reflects a lower local refractive index for the cation rich ionic layer in the EDL than for the anion rich counterpart, which was revealed by our recent study combining ESPR and molecular dynamics simulation [42]. After the negative shift, Δθ switched to a positive shift at potentials where the cathodic deposition occurs (<−0.7 V).…”
Section: -4 Simulation Of Resonance Angle Shiftmentioning
confidence: 78%
“…For the former, the Li UPD/UPS potentials are far negative from the potential of zero charge (PZC), where the EDL structure is in the "crowding" state and the first ionic layer is saturated with cations; therefore, the contribution of the EDL structure is too small and is neglected here. 26,50 For the latter, i.e., the contribution of the diffusion layer, the deposited/stripped Li amount is small with only about monatomic layer thickness, and in contrast, the concentration of Li + in the ILs is high enough to be regarded as constant during the Li UPD/UPS. The time derivative of Δθ SPR can be expressed as…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…In addition, Δθ SPR is also generally sensitive enough to the ionic concentration in the EDL ,, and the diffusion layer, , but this is not the case with the present Li UPD/UPS case. For the former, the Li UPD/UPS potentials are far negative from the potential of zero charge (PZC), where the EDL structure is in the “crowding” state and the first ionic layer is saturated with cations; therefore, the contribution of the EDL structure is too small and is neglected here. , For the latter, i.e., the contribution of the diffusion layer, the deposited/stripped Li amount is small with only about monatomic layer thickness, and in contrast, the concentration of Li + in the ILs is high enough to be regarded as constant during the Li UPD/UPS. The time derivative of Δθ SPR can be expressed as where V Li is the molar volume of Li metal, F is the Faraday constant, and i Li is the current density for the Li UPD/UPS processes.…”
Section: Results and Discussionmentioning
confidence: 99%
“…As described in the last paragraph, SPR is sensitive enough to detect the change in the electric double layer structure during the charging/discharging process. [30][31][32][33][34] Figure 11a shows the shift of SPR angle, ¦H (= H SPR ¹ H SPR,0 , where H SPR,0 is H SPR when the measurements are started) during CV measurements within the potential window at the interface between Au thin film and an ionic liquid. 31 The SPR angle changes in a sigmoidal manner, in response to a negative potential sweep, almost independent of the three scan rates.…”
Section: Electric Double Layermentioning
confidence: 99%