7 research outputs found
Ion Dynamics in Solid Electrolytes: NMR Reveals the Elementary Steps of Li<sup>+</sup> Hopping in the Garnet Li<sub>6.5</sub>La<sub>3</sub>Zr<sub>1.75</sub>Mo<sub>0.25</sub>O<sub>12</sub>
Garnet-type oxides are considered
to belong to the most attractive
solid Li<sup>+</sup> electrolytes. This is due to their wide electrochemical
stability window as well as their superior ionic conductivity, with
a Li-ion transference number of almost one. Usually ionic conductivities
are studied via impedance spectroscopy on a macroscopic length scale.
Time-domain NMR methods, however, have been used much less extensively
to shed light on the elementary hopping processes in highly conducting
oxide garnets. Here, we used NMR relaxometry and stimulated echo NMR
to study Li<sup>+</sup> self-diffusion in Li<sub>6.5</sub>La<sub>3</sub>Zr<sub>1.75</sub>Mo<sub>0.25</sub>O<sub>12</sub> (LLZMO), which served
as a model compound to collect information on the <sup>7</sup>Li spin
dynamics. It turned out that NMR spin–lattice relaxation (SLR)
recorded in both the laboratory and rotating frame of reference shows
features that seem to be a universal fingerprint for fast conducting
garnets that have been stabilized in their cubic modification. In
contrast to Al-doped garnet-type Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> that modifies the Li sublattice, in LLZMO the
Li sublattice remains intact, offering the possibility to get to the
bottom of Li-ion dynamics in LLZO-based garnets. Most importantly,
whereas NMR SLR rates measured at 194.3 MHz reflect an almost universal
behavior of local hoppings being thermally activated by only 0.151(3)
eV, the spin-lock technique (33.3̅ kHz) gives evidence of two
separate, overlapping rate peaks with activation energies on the order
of 0.29 eV for the elementary steps of Li-ion hopping. This points
to a less pronounced distribution of Li<sup>+</sup> jump rates on
the kilohertz time scale than has been observed for the Al-stabilized
LLZO samples. The NMR results obtained also entail information on
both the Li<sup>+</sup> diffusion coefficients and the shape of the
underlying motional correlation functions. The latter has been provided
by <sup>7</sup>Li NMR spin-alignment echo correlation spectroscopy
that also shows the involvement of 24d and 96h sites in Li<sup>+</sup> diffusion
Crystal Structure of Garnet-Related Li-Ion Conductor Li<sub>7–3<i>x</i></sub>Ga<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub>: Fast Li-Ion Conduction Caused by a Different Cubic Modification?
Li-oxide
garnets such as Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> (LLZO) are among the most promising candidates for
solid-state electrolytes to be used in next-generation Li-ion batteries.
The garnet-structured cubic modification of LLZO, showing space group <i>Ia</i>-3<i>d</i>, has to be stabilized with supervalent
cations. LLZO stabilized with Ga<sup>3+</sup> shows superior properties
compared to LLZO stabilized with similar cations; however, the reason
for this behavior is still unknown. In this study, a comprehensive
structural characterization of Ga-stabilized LLZO is performed by
means of single-crystal X-ray diffraction. Coarse-grained samples
with crystal sizes of several hundred micrometers are obtained by
solid-state reaction. Single-crystal X-ray diffraction results show
that Li<sub>7–3<i>x</i></sub>Ga<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> with <i>x</i> > 0.07 crystallizes in the acentric cubic space group <i>I</i>-43<i>d</i>. This is the first definite record
of this
cubic modification for LLZO materials and might explain the superior
electrochemical performance of Ga-stabilized LLZO compared to its
Al-stabilized counterpart. The phase transition seems to be caused
by the site preference of Ga<sup>3+</sup>. <sup>7</sup>Li NMR spectroscopy
indicates an additional Li-ion diffusion process for LLZO with space
group <i>I</i>-43<i>d</i> compared to space group <i>Ia</i>-3<i>d</i>. Despite all efforts undertaken to
reveal structure–property relationships for this class of materials,
this study highlights the potential for new discoveries
Crystal Structure of Garnet-Related Li-Ion Conductor Li<sub>7–3<i>x</i></sub>Ga<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub>: Fast Li-Ion Conduction Caused by a Different Cubic Modification?
Li-oxide
garnets such as Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> (LLZO) are among the most promising candidates for
solid-state electrolytes to be used in next-generation Li-ion batteries.
The garnet-structured cubic modification of LLZO, showing space group <i>Ia</i>-3<i>d</i>, has to be stabilized with supervalent
cations. LLZO stabilized with Ga<sup>3+</sup> shows superior properties
compared to LLZO stabilized with similar cations; however, the reason
for this behavior is still unknown. In this study, a comprehensive
structural characterization of Ga-stabilized LLZO is performed by
means of single-crystal X-ray diffraction. Coarse-grained samples
with crystal sizes of several hundred micrometers are obtained by
solid-state reaction. Single-crystal X-ray diffraction results show
that Li<sub>7–3<i>x</i></sub>Ga<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> with <i>x</i> > 0.07 crystallizes in the acentric cubic space group <i>I</i>-43<i>d</i>. This is the first definite record
of this
cubic modification for LLZO materials and might explain the superior
electrochemical performance of Ga-stabilized LLZO compared to its
Al-stabilized counterpart. The phase transition seems to be caused
by the site preference of Ga<sup>3+</sup>. <sup>7</sup>Li NMR spectroscopy
indicates an additional Li-ion diffusion process for LLZO with space
group <i>I</i>-43<i>d</i> compared to space group <i>Ia</i>-3<i>d</i>. Despite all efforts undertaken to
reveal structure–property relationships for this class of materials,
this study highlights the potential for new discoveries
Site Occupation of Ga and Al in Stabilized Cubic Li<sub>7–3(<i>x</i>+<i>y</i>)</sub>Ga<sub><i>x</i></sub>Al<sub><i>y</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> Garnets As Deduced from <sup>27</sup>Al and <sup>71</sup>Ga MAS NMR at Ultrahigh Magnetic Fields
Li-containing garnets, which are
stabilized in their cubic modification
by doping with Al or Ga, show very high Li-ion conductivities. This
property qualifies them to be used as solid electrolytes in advanced
all-solid-state batteries. The relation between local structures and
dynamic properties, however, is still not fully understood. Here,
cubic mixed-doped Li<sub>7–3(<i>x</i>+<i>y</i>)</sub>Ga<sub><i>x</i></sub>Al<sub><i>y</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> garnet solid solutions
with different portions of Al and Ga were synthesized. It turned out
that the solubility of Ga is higher than that of Al; the evaluation
of 42 different doping compositions indicated an increase of the lattice
parameter <i>a</i><sub>0</sub> with increasing Ga content. <sup>71</sup>Ga MAS NMR spectra recorded at 21.1 T revealed two <sup>71</sup>Ga NMR resonances, corresponding to Ga occupying both the 24<i>d</i> (243 ppm) and 96<i>h</i> sites (193 ppm). This
behavior, which has been observed for the first time in this study,
is very similar to that of Al. The <sup>71</sup>Ga NMR line at 193
ppm observed here remained invisible in previous NMR studies that
were carried out at lower magnetic fields. The invisibility at lower
field is because of large second-order quadrupolar broadening that
has a lower effect on the <sup>71</sup>Ga NMR spectra at higher magnetic
field. Most importantly, the similarity in site preference of Al and
Ga found here inevitably raises a question about the significance
of a blocking effect on long-range Li-ion transport. It weakens the
assumption that the site preference of dopants is responsible for
the higher Li diffusivity of Ga-doped samples compared to the Al-doped
analogues. Concerning Li-ion dynamics, our <sup>7</sup>Li NMR line
shape measurements indicate that the change in lattice constant <i>a</i><sub>0</sub> with increasing doping level seems to have
a larger influence on Li-ion dynamics than the Al:Ga ratio
Synthesis, Crystal Chemistry, and Electrochemical Properties of Li<sub>7–2<i>x</i></sub>La<sub>3</sub>Zr<sub>2–<i>x</i></sub>Mo<sub><i>x</i></sub>O<sub>12</sub> (<i>x</i> = 0.1–0.4): Stabilization of the Cubic Garnet Polymorph via Substitution of Zr<sup>4+</sup> by Mo<sup>6+</sup>
Cubic Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> (LLZO) garnets are exceptionally well
suited to be used as solid electrolytes or protecting layers in “Beyond
Li-ion Battery” concepts. Unfortunately, cubic LLZO is not
stable at room temperature (RT) and has to be stabilized by supervalent
dopants. In this study we demonstrate a new possibility to stabilize
the cubic phase at RT via substitution of Zr<sup>4+</sup> by Mo<sup>6+</sup>. A Mo<sup>6+</sup> content of 0.25 per formula unit (pfu)
stabilizes the cubic LLZO phase, and the solubility limit is about
0.3 Mo<sup>6+</sup> pfu. Based on the results of neutron powder diffraction
and Raman spectroscopy, Mo<sup>6+</sup> is located at the octahedrally
coordinated 16<i>a</i> site of the cubic garnet structure
(space group <i>Ia</i>-3<i>d</i>). Since Mo<sup>6+</sup> has a smaller ionic radius compared to Zr<sup>4+</sup> the
lattice parameter <i>a</i><sub>0</sub> decreases almost
linearly as a function of the Mo<sup>6+</sup> content. The highest
bulk Li-ion conductivity is found for the 0.25 pfu composition, with
a typical RT value of 3.4 × 10<sup>–4</sup> S cm<sup>–1</sup>. An additional significant resistive contribution originating from
the sample interior (most probably from grain boundaries) could be
identified in impedance spectra. The latter strongly depends on the
prehistory and increases significantly after annealing at 700 °C
in ambient air. Cyclic voltammetry experiments on cells containing
Mo<sup>6+</sup> substituted LLZO indicate that the material is stable
up to 6 V
Fast Li-Ion-Conducting Garnet-Related Li<sub>7–3<i>x</i></sub>Fe<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> with Uncommon <i>I</i>4̅3<i>d</i> Structure
Fast
Li-ion-conducting Li oxide garnets receive a great deal of
attention as they are suitable candidates for solid-state Li electrolytes.
It was recently shown that Ga-stabilized Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> crystallizes in the acentric cubic space
group <i>I</i>4̅3<i>d</i>. This structure
can be derived by a symmetry reduction of the garnet-type <i>Ia</i>3̅<i>d</i> structure, which is the most
commonly found space group of Li oxide garnets and garnets in general.
In this study, single-crystal X-ray diffraction confirms the presence
of space group <i>I</i>4̅3<i>d</i> also
for Li<sub>7–3<i>x</i></sub>Fe<sub><i>x</i></sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub>. The crystal structure
was characterized by X-ray powder diffraction, single-crystal X-ray
diffraction, neutron powder diffraction, and Mößbauer
spectroscopy. The crystal–chemical behavior of Fe<sup>3+</sup> in Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> is very
similar to that of Ga<sup>3+</sup>. The symmetry reduction seems to
be initiated by the ordering of Fe<sup>3+</sup> onto the tetrahedral
Li1 (12<i>a</i>) site of space group <i>I</i>4̅3<i>d</i>. Electrochemical impedance spectroscopy measurements showed
a Li-ion bulk conductivity of up to 1.38 × 10<sup>–3</sup> S cm<sup>–1</sup> at room temperature, which is among the
highest values reported for this group of materials
Synthesis, Crystal Structure, and Stability of Cubic Li<sub>7–<i>x</i></sub>La<sub>3</sub>Zr<sub>2–<i>x</i></sub>Bi<sub><i>x</i></sub>O<sub>12</sub>
Li oxide garnets
are among the most promising candidates for solid-state electrolytes
in novel Li ion and Li metal based battery concepts. Cubic Li<sub>7</sub>La<sub>3</sub>Zr<sub>2</sub>O<sub>12</sub> stabilized by a
partial substitution of Zr<sup>4+</sup> by Bi<sup>5+</sup> has not
been the focus of research yet, despite the fact that Bi<sup>5+</sup> would be a cost-effective alternative to other stabilizing cations
such as Nb<sup>5+</sup> and Ta<sup>5+</sup>. In this study, Li<sub>7–<i>x</i></sub>La<sub>3</sub>Zr<sub>2–<i>x</i></sub>Bi<sub><i>x</i></sub>O<sub>12</sub> (<i>x</i> = 0.10, 0.20, ..., 1.00) was prepared by a low-temperature
solid-state synthesis route. The samples have been characterized by
a rich portfolio of techniques, including scanning electron microscopy,
X-ray powder diffraction, neutron powder diffraction, Raman spectroscopy,
and <sup>7</sup>Li NMR spectroscopy. Pure-phase cubic garnet samples
were obtained for <i>x</i> ≥ 0.20. The introduction
of Bi<sup>5+</sup> leads to an increase in the unit-cell parameters.
Samples are sensitive to air, which causes the formation of LiOH and
Li<sub>2</sub>CO<sub>3</sub> and the protonation of the garnet phase,
leading to a further increase in the unit-cell parameters. The incorporation
of Bi<sup>5+</sup> on the octahedral 16<i>a</i> site was
confirmed by Raman spectroscopy. <sup>7</sup>Li NMR spectroscopy shows
that fast Li ion dynamics are only observed for samples with high
Bi<sup>5+</sup> contents