TY - JOUR
T1 - Perovskite Na-ion conductors developed from analogous Li3xLa2/3−xTiO3(LLTO)
T2 - chemo-mechanical and defect engineering
AU - Lin, Yu Ying
AU - Gustafson, William J.
AU - Murray, Shannon E.
AU - Shoemaker, Daniel P.
AU - Ertekin, Elif
AU - Krogstad, Jessica A.
AU - Perry, Nicola H.
N1 - Funding Information:
This material is primarily based upon work supported by the US Army CERL W9132T-19-2-0008 (to E. E., J. A. K. and N. H. P., also supporting Y. Y. L.). D. P. S. acknowledges research support by the Army Research Office under Grant Number W911NF-17-1-0142. S. E. M. acknowledges support from the National Science Foundation Graduate Research Fellowship Program under Grant No. DGE1144245. XRD, SEM, and sputter coating were carried out in the Materials Research Laboratory Central Research Facilities, University of Illinois. The authors also acknowledge the use of XRD instrumentation supported by NSF through the University of Illinois Materials Research Science and Engineering Center DMR-1720633. Use of the Advanced Photon Source at Argonne National Laboratory was supported by the U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. The authors would like to thank Dr Charles Smith and Dr Nathan Madden (University of Illinois at Urbana-Champaign) for their help with using spark plasma sintering as an alternative route to densify the pellet.
Publisher Copyright:
© The Royal Society of Chemistry 2021.
PY - 2021/10/7
Y1 - 2021/10/7
N2 - Na-ion conducting solid electrolytes can enable both the enhanced safety profile of all-solid-state-batteries and the transition to an earth-abundant charge-carrier for large-scale stationary storage. In this work, we developed new perovskite-structured Na-ion conductors from the analogous fast Li-ion conducting Li3xLa2/3−xTiO3(LLTO), testing strategies of chemo-mechanical and defect engineering. NaxLa2/3−1/3xZrO3(NLZ) and NaxLa1/3−1/3xBa0.5ZrO3(NLBZ) were prepared using a modified Pechini method with varying initial stoichiometries and sintering temperatures. With the substitution of larger framework cations Zr4+and Ba2+on B- and A-sites respectively, NLZ and NLBZ both had larger lattice parameters compared to LLTO, in order to accommodate and potentially enhance the transport of larger Na ions. Additionally, we sought to introduce Na vacancies through (a) sub-stoichiometric Na : La ratios, (b) Na loss during sintering, and (c) donor doping with Nb. AC impedance spectroscopy and DC polarization experiments were performed on both Na0.5La0.5ZrO3and Na0.25La0.25Ba0.5ZrO3in controlled gas environments (variable oxygen partial pressure, humidity) at elevated temperatures to quantify the contributions of various possible charge carriers (sodium ions, holes, electrons, oxygen ions, protons). Our results showed that the lattice-enlarged NLZ and NLBZ exhibited ∼19× (conventional sintering)/49× (spark plasma sintering) and ∼7× higher Na-ion conductivities, respectively, compared to unexpanded Na0.42La0.525TiO3. Moreover, the Na-ion conductivity of Na0.5La0.5ZrO3is comparable with that of NaNbO3, despite having half the carrier concentration. Additionally, more than 96% of the total conductivity in dry conditions was contributed by sodium ions for both compositions, with negligible electronic conductivity and little oxygen ion conductivity. We also identified factors that limited Na-ion transport: NLZ and NLBZ were both challenging to densify using conventional sintering without the loss of Na because of its volatility. With spark plasma sintering, higher density can be achieved. In addition, the NLZ perovskite phase appeared unable to accommodate significant Na deficiency, whereas NLBZ allowed some. Density functional theory calculations supported a thermodynamic limitation to creation of Na-deficient NLZ in favor of a pyrochlore-type phase. Humid environments generated different behavior: in Na0.25La0.25Ba0.5ZrO3, incorporated protons raised total conductivity, whereas in Na0.5La0.5ZrO3, they lowered total conductivity. Ultimately, this systematic approach revealed both effective approaches and limitations to achieving super-ionic Na-ion conductivity, which may eventually be overcome through alternative processing routes.
AB - Na-ion conducting solid electrolytes can enable both the enhanced safety profile of all-solid-state-batteries and the transition to an earth-abundant charge-carrier for large-scale stationary storage. In this work, we developed new perovskite-structured Na-ion conductors from the analogous fast Li-ion conducting Li3xLa2/3−xTiO3(LLTO), testing strategies of chemo-mechanical and defect engineering. NaxLa2/3−1/3xZrO3(NLZ) and NaxLa1/3−1/3xBa0.5ZrO3(NLBZ) were prepared using a modified Pechini method with varying initial stoichiometries and sintering temperatures. With the substitution of larger framework cations Zr4+and Ba2+on B- and A-sites respectively, NLZ and NLBZ both had larger lattice parameters compared to LLTO, in order to accommodate and potentially enhance the transport of larger Na ions. Additionally, we sought to introduce Na vacancies through (a) sub-stoichiometric Na : La ratios, (b) Na loss during sintering, and (c) donor doping with Nb. AC impedance spectroscopy and DC polarization experiments were performed on both Na0.5La0.5ZrO3and Na0.25La0.25Ba0.5ZrO3in controlled gas environments (variable oxygen partial pressure, humidity) at elevated temperatures to quantify the contributions of various possible charge carriers (sodium ions, holes, electrons, oxygen ions, protons). Our results showed that the lattice-enlarged NLZ and NLBZ exhibited ∼19× (conventional sintering)/49× (spark plasma sintering) and ∼7× higher Na-ion conductivities, respectively, compared to unexpanded Na0.42La0.525TiO3. Moreover, the Na-ion conductivity of Na0.5La0.5ZrO3is comparable with that of NaNbO3, despite having half the carrier concentration. Additionally, more than 96% of the total conductivity in dry conditions was contributed by sodium ions for both compositions, with negligible electronic conductivity and little oxygen ion conductivity. We also identified factors that limited Na-ion transport: NLZ and NLBZ were both challenging to densify using conventional sintering without the loss of Na because of its volatility. With spark plasma sintering, higher density can be achieved. In addition, the NLZ perovskite phase appeared unable to accommodate significant Na deficiency, whereas NLBZ allowed some. Density functional theory calculations supported a thermodynamic limitation to creation of Na-deficient NLZ in favor of a pyrochlore-type phase. Humid environments generated different behavior: in Na0.25La0.25Ba0.5ZrO3, incorporated protons raised total conductivity, whereas in Na0.5La0.5ZrO3, they lowered total conductivity. Ultimately, this systematic approach revealed both effective approaches and limitations to achieving super-ionic Na-ion conductivity, which may eventually be overcome through alternative processing routes.
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U2 - 10.1039/d1ta04252a
DO - 10.1039/d1ta04252a
M3 - Article
AN - SCOPUS:85116398639
VL - 9
SP - 21241
EP - 21258
JO - Journal of Materials Chemistry A
JF - Journal of Materials Chemistry A
SN - 2050-7488
IS - 37
ER -