Ab Initio Simulations and Electronic Structure of Lithium-Doped Ionic Liquids: Structure, Transport, and Electrochemical Stability.
Density functional theory (DFT), density functional theory molecular dynamics (DFT-MD), and classical molecular dynamics using polarizable force fields (PFF-MD) are employed to evaluate the influence of Li(+) on the structure, transport, and electrochemical stability of three potential ionic liquid electrolytes: N-methyl-N-butylpyrrolidinium bis(trifluoromethanesulfonyl)imide ([pyr14][TFSI]), N-methyl-N-propylpyrrolidinium bis(fluorosulfonyl)imide ([pyr13][FSI]), and 1-ethyl-3-methylimidazolium boron tetrafluoride ([EMIM][BF4]). We characterize the Li(+) solvation shell through DFT computations of [Li(Anion)n]((n-1)-) clusters, DFT-MD simulations of isolated Li(+) in small ionic liquid systems, and PFF-MD simulations with high Li-doping levels in large ionic liquid systems. At low levels of Li-salt doping, highly stable solvation shells having two to three anions are seen in both [pyr14][TFSI] and [pyr13][FSI], whereas solvation shells with four anions dominate in [EMIM][BF4]. At higher levels of doping, we find the formation of complex Li-network structures that increase the frequency of four anion-coordinated solvation shells. A comparison of computational and experimental Raman spectra for a wide range of [Li(Anion)n]((n-1)-) clusters shows that our proposed structures are consistent with experiment. We then compute the ion diffusion coefficients and find measures from small-cell DFT-MD simulations to be the correct order of magnitude, but influenced by small system size and short simulation length. Correcting for these errors with complementary PFF-MD simulations, we find DFT-MD measures to be in close agreement with experiment. Finally, we compute electrochemical windows from DFT computations on isolated ions, interacting cation/anion pairs, and liquid-phase systems with Li-doping. For the molecular-level computations, we generally find the difference between ionization energy and electron affinity from isolated ions and interacting cation/anion pairs to provide upper and lower bounds, respectively, to experiment. In the liquid phase, we find the difference between the lowest unoccupied and highest occupied electronic levels in pure and hybrid functionals to provide lower and upper bounds, respectively, to experiment. Li-doping in the liquid-phase systems results in electrochemical windows little changed from the neat systems.
AMA Inc., Thermal Protection Materials Branch, Mail Stop 234-1, ‡Entry Systems and Technology Division, Mail Stop 230-3, and §Thermal Protection Materials Branch, Mail Stop 234-1, NASA Ames Research Center , Moffett Field, California 94035, United States.
Justin B
JB
Haskins
AMA Inc., Thermal Protection Materials Branch, Mail Stop 234-1, ‡Entry Systems and Technology Division, Mail Stop 230-3, and §Thermal Protection Materials Branch, Mail Stop 234-1, NASA Ames Research Center , Moffett Field, California 94035, United States.
Charles W
CW
Bauschlicher
AMA Inc., Thermal Protection Materials Branch, Mail Stop 234-1, ‡Entry Systems and Technology Division, Mail Stop 230-3, and §Thermal Protection Materials Branch, Mail Stop 234-1, NASA Ames Research Center , Moffett Field, California 94035, United States.
John W
JW
Lawson
D004563:Electrochemistry; D052578:Ionic Liquids / Q000737:chemistry*; D008094:Lithium / Q000737:chemistry*; D056004:Molecular Dynamics Simulation
D052578:Ionic Liquids; D008094:Lithium