5 research outputs found
Structural Evolution and Li Dynamics in Nanophase Li<sub>3</sub>PS<sub>4</sub> by Solid-State and Pulsed-Field Gradient NMR
The ceramic lithium ion conductor
β-Li<sub>3</sub>PS<sub>4</sub> has a disordered and nanoporous
structure that leads to an
enhancement in ionic conductivity by some 3 orders of magnitude compared
to the crystalline γ phase. The β phase is prepared by
thermal treatment of an inorganic–organic complex based on
Li<sub>3</sub>PS<sub>4</sub> and THF. Multinuclear (<sup>1</sup>H, <sup>6,7</sup>Li, <sup>31</sup>P) solid-state NMR spectroscopy is used
to characterize the structural phase evolution of the starting material
at various steps in the thermal treatment. The β phase formed
after high temperature treatment is recognized as spectroscopically
distinct from the bulk γ-Li<sub>3</sub>PS<sub>4</sub> compound.
Also formed is an amorphous lithium thiophosphate phase that is metastable
as verified by annealing over an extended period. Lithium ion self-diffusion
coefficients are measurable by standard pulsed-field gradient NMR
methods at 100 °C and with values consistent with the high ionic
conductivity previously reported for this material
Influence of Solvent on Ion Aggregation and Transport in PY<sub>15</sub>TFSI Ionic Liquid–Aprotic Solvent Mixtures
Molecular dynamics (MD) simulations
using a many-body polarizable
APPLE&P force field have been performed on mixtures of the <i>N</i>-methyl-<i>N</i>-pentylpyrrolidinium bisÂ(trifluoromethanesulfonyl)Âimide
(PY<sub>15</sub>TFSI) ionic liquid (IL) with three molecular solvents:
propylene carbonate (PC), dimethyl carbonate (DMC), and acetonitrile
(AN). The MD simulations predict density, viscosity, and ionic conductivity
values that agree well with the experimental results. In the solvent-rich
regime, the ionic conductivity of the PY<sub>15</sub>TFSI–AN
mixtures was found to be significantly higher than the conductivity
of the corresponding −PC and −DMC mixtures, despite
the similar viscosity values obtained from both the MD simulations
and experiments for the −DMC and −AN mixtures. The significantly
lower conductivity of the PY<sub>15</sub>TFSI–DMC mixtures,
as compared to those for PY<sub>15</sub>TFSI–AN, in the solvent-rich
regime was attributed to the more extensive ion aggregation observed
for the −DMC mixtures. The PY<sub>15</sub>TFSI–DMC mixtures
present an interesting case where the addition of the organic solvent
to the IL results in an increase in the cation–anion correlations,
in contrast to what is found for the mixtures with PC and AN, where
ion motion became increasingly uncorrelated with addition of solvent.
A combination of pfg-NMR and conductivity measurements confirmed the
MD simulation predictions. Further insight into the molecular interactions
and properties was also obtained using the MD simulations by examining
the solvent distribution in the IL–solvent mixtures and the
mixture excess properties
Diffusion Coefficients from <sup>13</sup>C PGSE NMR MeasurementsFluorine-Free Ionic Liquids with the DCTA<sup>–</sup> Anion
Pulsed-field gradient spin–echo (PGSE) NMR is
a widely used
method for the determination of molecular and ionic self-diffusion
coefficients. The analysis has thus far been limited largely to <sup>1</sup>H, <sup>7</sup>Li, <sup>19</sup>F, and <sup>31</sup>P nuclei.
This limitation handicaps the analysis of materials without these
nuclei or for which these nuclei are insufficient for complete characterization.
This is demonstrated with a class of ionic liquids (or ILs) based
on the nonfluorinated anion 4,5-dicarbonitrile-1,2,3-triazole (DCTA<sup>–</sup>). It is demonstrated here that <sup>13</sup>C-PGSE
NMR can be used to both verify the diffusion coefficients obtained
from other nuclei, as well as characterize materials that lack commonly
scrutinized nuclei î—¸ all without the need for specialized NMR
methods
An Iodide-Based Li<sub>7</sub>P<sub>2</sub>S<sub>8</sub>I Superionic Conductor
In
an example of stability from instability, a Li<sub>7</sub>P<sub>2</sub>S<sub>8</sub>I solid-state Li-ion conductor derived from β-Li<sub>3</sub>PS<sub>4</sub> and LiI demonstrates electrochemical stability
up to 10 V vs Li/Li<sup>+</sup>. The oxidation instability of I is
subverted via its incorporation into the coordinated structure. The
inclusion of I also creates stability with the metallic Li anode while
simultaneously enhancing the interfacial kinetics and ionic conductivity.
Low-temperature membrane processability enables facile fabrication
of dense membranes, making this conductor suitable for industrial
adoption
Liquid Structure with Nano-Heterogeneity Promotes Cationic Transport in Concentrated Electrolytes
Using
molecular dynamics simulations, small-angle neutron scattering,
and a variety of spectroscopic techniques, we evaluated the ion solvation
and transport behaviors in aqueous electrolytes containing bisÂ(trifluoromethanesulfonyl)Âimide.
We discovered that, at high salt concentrations (from 10 to 21 mol/kg),
a disproportion of cation solvation occurs, leading to a liquid structure
of heterogeneous domains with a characteristic length scale of 1 to
2 nm. This unusual nano-heterogeneity effectively decouples cations
from the Coulombic traps of anions and provides a 3D percolating lithium–water
network, <i>via</i> which 40% of the lithium cations are
liberated for fast ion transport even in concentration ranges traditionally
considered too viscous. Due to such percolation networks, superconcentrated
aqueous electrolytes are characterized by a high lithium-transference
number (0.73), which is key to supporting an assortment of battery
chemistries at high rate. The in-depth understanding of this transport
mechanism establishes guiding principles to the tailored design of
future superconcentrated electrolyte systems