Please use this identifier to cite or link to this item: http://hdl.handle.net/2381/44415
Title: Free and Bound States of Ions in Ionic Liquids, Conductivity, and Underscreening Paradox
Authors: Brilliantov, N
Guang, G
Chen, M
Bi, S
Goodwin, Z
Postnikov, E
Urbakh, M
Kornyshev, A
First Published: 6-May-2019
Publisher: American Physical Society
Citation: Physical Review X, 2019, 9, pp. 021024-1-021024-22 (22)
Abstract: Using molecular dynamics simulations and theoretical analysis of velocity-autocorrelation functions, we study ion transport mechanisms in typical room-temperature ionic liquids. We show that ions may reside in two states: free and bound with an interstate exchange. We investigate quantitatively the exchange process and reveal new qualitative features of this process. To this end, we propose a dynamic criterion for free and bound ions based on the ion trajectory density and demonstrate that this criterion is consistent with a static one based on interionic distances. Analyzing the trajectories of individual cations and anions, we estimate the time that ions spend in bound “clustered states” and when they move quasifreely. Using this method, we evaluate the average portion of “free” ions as approximately 15%–25%, increasing with temperature in the range of 300–600 K. The ion diffusion coefficients and conductivities as a function of the temperature calculated from the velocity and electrical-current autocorrelation functions reproduce the reported experimental data very well. The experimental data for the direct-current conductivity (constant ionic current) is in good agreement with theoretical predictions of the Nernst-Einstein equation based on the concentrations and diffusion coefficients of free ions obtained in our simulations. In analogy with electronic semiconductors, we scrutinize an “ionic semiconductor” model for ionic liquids, with valence and conduction “bands” for ions separated by an energy gap. The obtained band gap for the ionic liquid is small, around 26 meV, allowing for easy interchange between the two dynamic states. Moreover, we discuss the underscreening paradox in the context of the amount of free charge carriers, showing that the obtained results do not yet approve its simplistic resolution.
DOI Link: 10.1103/PhysRevX.9.021024
eISSN: 2160-3308
Links: https://journals.aps.org/prx/abstract/10.1103/PhysRevX.9.021024
http://hdl.handle.net/2381/44415
Version: Publisher Version
Status: Peer-reviewed
Type: Journal Article
Rights: Copyright © the authors, 2019. This is an open-access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Description: See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevX.9.021024 for (1) comparison of results for the temperature-dependent percentage of free ions obtained by three different methods; (2) detailed study of the kinetics of exchange process characterized through survival probabilities for anions in [Bmim][TFSI]; (3) additional analysis of the velocityautocorrelation functions (VACFs) and diffusion coefficients; (4) demonstration of how (exceptionally) well the two state theory developed in the main text can fit the simulated VACFs for anions in [Bmim][TFSI]; (5) analysis of the temperature effect on electric-current autocorrelation function (ECACF) and its Fourier spectrum; (6) analysis of ECACFs and the corresponding values of electrical conductivities obtained by integration of ECAFCs over time; additional information on the results obtained for two other RTILs [Emim][TFSI] and [Bmim] [PF6], including the temperature-dependent (7) percentage of free ions and (8) conductivities; (9) study of the effect of the simulation system size on the ion diffusion coefficient.
Appears in Collections:Published Articles, Dept. of Mathematics

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