journal article·2020-08-20Open access

Structural and Dynamical Properties of Potassium Dodecahydro-monocarba-closo-dodecaborate: KCB11H12

Mirjana Dimitrievska, Hui Wu, Vitalie Stavila, Olga A. Babanova, Roman V. Skoryunov, Alexei V. Soloninin, Wei Zhou, Benjamin A. Trump, Mikael S. Andersson, Alexander V. Skripov, Terrence J. Udovic

The Journal of Physical Chemistry C· Volume 124· Issue 33

Abstract

MCB 11 H 12 (M: Li, Na) dodecahydro-monocarba- closo -dodecaborate salt compounds are known to have stellar superionic Li + and Na + conductivities in their high-temperature disordered phases, making them potentially appealing electrolytes in all-solid-state batteries. Nonetheless, it is of keen interest to search for other related materials with similar conductivities while at the same time exhibiting even lower (more device-relevant) disordering temperatures, a key challenge for this class of materials. With this in mind, the unknown structural and dynamical properties of the heavier KCB 11 H 12 congener were investigated in detail by X-ray powder diffraction, differential scanning calorimetry, neutron vibrational spectroscopy, nuclear magnetic resonance, quasielastic neutron scattering, and AC impedance measurements. This salt indeed undergoes an entropy-driven, reversible, order–disorder transformation and with a lower onset temperature (348 K upon heating and 340 K upon cooling) in comparison to the lighter LiCB 11 H 12 and NaCB 11 H 12 analogues. The K + cations in both the low- T ordered monoclinic ( P 2 1 / c ) and high- T disordered cubic ( Fm 3̅ m ) structures occupy octahedral interstices formed by CB 11 H 12 – anions. In the low- T structure, the anions orient themselves so as to avoid close proximity between their highly electropositive C–H vertices and the neighboring K + cations. In the high- T structure, the anions are orientationally disordered, although to best avoid the K + cations, the anions likely orient themselves so that their C–H axes are aligned in one of eight possible directions along the body diagonals of the cubic unit cell. Across the transition, anion reorientational jump rates change from 6.2 × 10 6 s –1 in the low- T phase (332 K) to 2.6 × 10 10 s –1 in the high- T phase (341 K). In tandem, K + conductivity increases by about 30-fold across the transition, yielding a high- T phase value of 3.2 × 10 –4 S cm –1 at 361 K. However, this is still about 1 to 2 orders of magnitude lower than that observed for LiCB 11 H 12 and NaCB 11 H 12, suggesting that the relatively larger K + cation is much more sterically hindered than Li + and Na + from diffusing through the anion lattice via the network of smaller interstitial sites.
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Research context

OpenAlex topics: Boron Compounds in Chemistry · Radioactive element chemistry and processing · Chemical Synthesis and Characterization

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899-6102, United States

National Renewable Energy Laboratory, Golden, Colorado 80401, United States

Institute of Materials, Faculty of Engineering, École Polytechnique Fedérale de Lausanne, Lausanne 1015, Switzerland

Energy Nanomaterials, Sandia National Laboratories, Livermore, California 94551, United States

Institute of Metal Physics, Ural Branch of the Russian Academy of Sciences, Ekaterinburg 620108, Russia

Department of Chemistry and Chemical Engineering, Chalmers University of Technology, Göteborg SE-412 96, Sweden

Department of Materials Science and Engineering, University of Maryland, College Park, Maryland 20742-2115, United States

Funding

Vetenskapsrådet · Russian Science Foundation · U.S. Department of Energy

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