4 research outputs found
Legislative Documents
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High Capacity Garnet-Based All-Solid-State Lithium Batteries: Fabrication and 3D-Microstructure Resolved Modeling
The
development of high-capacity, high-performance all-solid-state batteries
requires the specific design and optimization of its components, especially
on the positive electrode side. For the first time, we were able to
produce a completely inorganic mixed positive electrode consisting
only of LiCoO<sub>2</sub> and Ta-substituted Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> (LLZ:Ta) without the use of additional
sintering aids or conducting additives, which has a high theoretical
capacity density of 1 mAh/cm<sup>2</sup>. A true all-solid-state cell
composed of a Li metal negative electrode, a LLZ:Ta garnet electrolyte,
and a 25 μm thick LLZ:Ta + LiCoO<sub>2</sub> mixed positive
electrode was manufactured and characterized. The cell shows 81% utilization
of theoretical capacity upon discharging at elevated temperatures
and rather high discharge rates of 0.1 mA (0.1 C). However, even though
the room temperature performance is also among the highest reported
so far for similar cells, it still falls far short of the theoretical
values. Therefore, a 3D reconstruction of the manufactured mixed positive
electrode was used for the first time as input for microstructure-resolved
continuum simulations. The simulations are able to reproduce the electrochemical
behavior at elevated temperature favorably, however fail completely
to predict the performance loss at room temperature. Extensive parameter
studies were performed to identify the limiting processes, and as
a result, interface phenomena occurring at the cathode active material/solid–electrolyte
interface were found to be the most probable cause for the low performance
at room temperature. Furthermore, the simulations are used for a sound
estimation of the optimization potential that can be realized with
this type of cell, which provides important guidelines for future
oxide based all-solid-state battery research and fabrication
Scandium-Substituted Na<sub>3</sub>Zr<sub>2</sub>(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) Prepared by a Solution-Assisted Solid-State Reaction Method as Sodium-Ion Conductors
As possible electrolyte materials
for all-solid-state Na-ion batteries
(NIBs), scandium-substituted Na<sub>3</sub>Zr<sub>2</sub>Â(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) in the structure of NASICONs
(Na superionic conductors) has received hardly any attention so far,
although among all the trivalent cations, Sc<sup>3+</sup> might be
the most suitable substitution ion for Na<sub>3</sub>Zr<sub>2</sub>(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) because the ionic radius
of Sc<sup>3+</sup> (74.5 pm) is the closest to that of Zr<sup>4+</sup> (72.0 pm). In this study, a solution-assisted solid-state reaction
(SASSR) method is described, and a series of scandium-substituted
Na<sub>3</sub>Zr<sub>2</sub>(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) with the formula of Na<sub>3+<i>x</i></sub>Sc<sub><i>x</i></sub>Zr<sub>2‑<i>x</i></sub>(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) (NSZSP<i>x</i>, 0
≤ <i>x</i> ≤ 0.6) have been prepared. This
synthesis route can be applied for powder preparation on a large scale
and at low cost. With increasing degrees of scandium substitution,
the total conductivity of the samples also increases. An optimum total
Na-ion conductivity of 4.0 × 10<sup>–3</sup> S cm<sup>–1</sup> at 25 °C is achieved by Na<sub>3.4</sub>Sc<sub>0.4</sub>Zr<sub>1.6</sub>Â(SiO<sub>4</sub>)<sub>2</sub>(PO<sub>4</sub>) (NSZSP0.4), which is the best value of all reported polycrystalline
Na-ion conductors. The possible reasons for such high conductivity
are discussed
Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> Interface Modification for Li Dendrite Prevention
Al-contaminated Ta-substituted Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> (LLZ:Ta), synthesized
via solid-state reaction, and Al-free Ta-substituted Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub>, fabricated by hot-press
sintering (HP-LLZ:Ta), have relative densities of 92.7% and 99.0%,
respectively. Impedance spectra show the total conductivity of LLZ:Ta
to be 0.71 mS cm<sup>–1</sup> at 30 °C and that of HP-LLZ:Ta
to be 1.18 mS cm<sup>–1</sup>. The lower total conductivity
for LLZ:Ta than HP-LLZ:Ta was attributed to the higher grain boundary
resistance and lower relative density of LLZ:Ta, as confirmed by their
microstructures. Constant direct current measurements of HP-LLZ:Ta
with a current density of 0.5 mA cm<sup>–2</sup> suggest that
the short circuit formation was neither due to the low relative density
of the samples nor the reduction of Li–Al glassy phase at grain
boundaries. TEM, EELS, and MAS NMR were used to prove that the short
circuit was from Li dendrite formation inside HP-LLZ:Ta, which took
place along the grain boundaries. The Li dendrite formation was found
to be mostly due to the inhomogeneous contact between LLZ solid electrolyte
and Li electrodes. By flatting the surface of the LLZ:Ta pellets and
using thin layers of Au buffer to improve the contact between LLZ:Ta
and Li electrodes, the interface resistance could be dramatically
reduced, which results in short-circuit-free cells when running a
current density of 0.5 mA cm<sup>–2</sup> through the pellets.
Temperature-dependent stepped current density galvanostatic cyclings
were also carried out to determine the critical current densities
for the short circuit formation. The short circuit that still occurred
at higher current density is due to the inhomogeneous dissolution
and deposition of metallic Li at the interfaces of Li electrodes and
LLZ solid electrolyte when cycling the cell at large current densities