28 research outputs found
Divalent Iron Nitridophosphates: A New Class of Cathode Materials for Li-Ion Batteries
Divalent Iron Nitridophosphates: A New Class of Cathode
Materials for Li-Ion Batterie
Probing Reversible Multielectron Transfer and Structure Evolution of Li<sub>1.2</sub>Cr<sub>0.4</sub>Mn<sub>0.4</sub>O<sub>2</sub> Cathode Material for Li-Ion Batteries in a Voltage Range of 1.0–4.8 V
Li<sub>1.2</sub>Cr<sub>0.4</sub>Mn<sub>0.4</sub>O<sub>2</sub> (0.4LiCrO<sub>2</sub>·0.4Li<sub>2</sub>MnO<sub>3</sub>) is an interesting
intercalation-type cathode material with high theoretical capacity
of 387 mAh g<sup>–1</sup> based on multiple-electron transfer
of Cr<sup>3+</sup>/Cr<sup>6+</sup>. In this work, it has been demonstrated
that the reversible Cr<sup>3+</sup>/Cr<sup>6+</sup> redox reaction
can only be realized in a wide voltage range between 1.0 and 4.8 V.
This is mainly due to large polarization during the discharge. The
reversible migration of the Cr ions between octahedral and tetrahedral
sites leads to large extent of cation mixing between lithium and transition
metal layers, which does not affect the lithium storage capacity and
stabilize the structure. In addition, a distorted spinel phase (Li<sub>3</sub>M<sub>2</sub>O<sub>4</sub>) is identified in the deeply discharged
sample (1.0 V, Li<sub>1.5</sub>Cr<sub>0.4</sub>Mn<sub>0.4</sub>O<sub>2</sub>). The above results can explain the high reversible capacity
and high structural stability achieved on Li<sub>1.2</sub>Cr<sub>0.4</sub>Mn<sub>0.4</sub>O<sub>2</sub>. These new findings will provide further
in depth understanding on multielectron transfer and local structure
stabilization mechanisms in intercalation chemistry, which are essential
for understanding and developing a high capacity intercalation-type
cathode for next generation high energy density Li-ion batteries
Oxygen-Release-Related Thermal Stability and Decomposition Pathways of Li<sub><i>x</i></sub>Ni<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> Cathode Materials
The thermal stability of charged
cathode materials is one of the
critical properties affecting the safety characteristics of lithium-ion
batteries. New findings on the thermal-stability and thermal-decomposition
pathways related to the oxygen release are discovered for the high-voltage
spinel Li<sub><i>x</i></sub>Ni<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> (LNMO) with ordered (<i>o</i>-) and disordered
(<i>d</i>-) structures at the fully delithiated (charged)
state using a combination of in situ time-resolved X-ray diffraction
(TR-XRD) coupled with mass spectroscopy (MS) and X-ray absorption
spectroscopy (XAS) during heating. Both <i>o</i>- and <i>d</i>- Li<sub><i>x</i></sub>Ni<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub>, at their fully charged states, start oxygen-releasing
structural changes at temperatures below 300 °C, which is in
sharp contrast to the good thermal stability of the 4V-spinel Li<sub><i>x</i></sub>Mn<sub>2</sub>O<sub>4</sub> with no oxygen
being released up to 375 °C. This is mainly caused by the presence
of Ni<sup>4+</sup> in LNMO, which undergoes dramatic reduction during
the thermal decomposition. In addition, charged <i>o</i>-LNMO shows better thermal stability than the <i>d</i>-LNMO
counterpart, due to the Ni/Mn ordering and smaller amount of the rock-salt
impurity phase in <i>o</i>-LNMO. Two newly identified thermal-decomposition
pathways from the initial Li<sub><i>x</i></sub>Ni<sub>0.5</sub>Mn<sub>1.5</sub>O<sub>4</sub> spinel to the final NiMn<sub>2</sub>O<sub>4</sub>-type spinel structure with and without the intermediate
phases (NiMnO<sub>3</sub> and α-Mn<sub>2</sub>O<sub>3</sub>)
are found to play key roles in thermal stability and oxygen release
of LNMO during thermal decomposition
Quantification of Honeycomb Number-Type Stacking Faults: Application to Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> Cathodes for Na-Ion Batteries
Ordered and disordered samples of
honeycomb-lattice Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> were
investigated as cathodes for Na-ion batteries, and it was determined
that the ordered sample exhibits better electrochemical performance,
with a specific capacity of 104 mA h/g delivered at plateaus of 3.5
and 3.2 V (vs Na<sup>+</sup>/Na) with minimal capacity fade during
extended cycling. Advanced imaging and diffraction investigations
showed that the primary difference between the ordered and disordered
samples is the amount of number-type stacking faults associated with
the three possible centering choices for each honeycomb layer. A labeling
scheme for assigning the number position of honeycomb layers is described,
and it is shown that the translational shift vectors between layers
provide the simplest method for classifying different repeat patterns.
It is demonstrated that the number position of honeycomb layers can
be directly determined in high-angle annular dark-field scanning transmission
electron microscopy (STEM-HAADF) imaging studies. By the use of fault
models derived from STEM studies, it is shown that both the sharp,
symmetric subcell peaks and the broad, asymmetric superstructure peaks
in powder diffraction patterns can be quantitatively modeled. About
20% of the layers in the ordered monoclinic sample are faulted in
a nonrandom manner, while the disordered sample stacking is not fully
random but instead contains about 4% monoclinic order. Furthermore,
it is shown that the ordered sample has a series of higher-order superstructure
peaks associated with 6-, 9-, 12-, and 15-layer periods whose existence
is transiently driven by the presence of long-range strain that is
an inherent consequence of the synthesis mechanism revealed through
the present diffraction and imaging studies. This strain is closely
associated with a monoclinic shear that can be directly calculated
from cell lattice parameters and is strongly correlated with the degree
of ordering in the samples. The present results are broadly applicable
to other honeycomb-lattice systems, including Li<sub>2</sub>MnO<sub>3</sub> and related Li-excess cathode compositions
Quantification of Honeycomb Number-Type Stacking Faults: Application to Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> Cathodes for Na-Ion Batteries
Ordered and disordered samples of
honeycomb-lattice Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> were
investigated as cathodes for Na-ion batteries, and it was determined
that the ordered sample exhibits better electrochemical performance,
with a specific capacity of 104 mA h/g delivered at plateaus of 3.5
and 3.2 V (vs Na<sup>+</sup>/Na) with minimal capacity fade during
extended cycling. Advanced imaging and diffraction investigations
showed that the primary difference between the ordered and disordered
samples is the amount of number-type stacking faults associated with
the three possible centering choices for each honeycomb layer. A labeling
scheme for assigning the number position of honeycomb layers is described,
and it is shown that the translational shift vectors between layers
provide the simplest method for classifying different repeat patterns.
It is demonstrated that the number position of honeycomb layers can
be directly determined in high-angle annular dark-field scanning transmission
electron microscopy (STEM-HAADF) imaging studies. By the use of fault
models derived from STEM studies, it is shown that both the sharp,
symmetric subcell peaks and the broad, asymmetric superstructure peaks
in powder diffraction patterns can be quantitatively modeled. About
20% of the layers in the ordered monoclinic sample are faulted in
a nonrandom manner, while the disordered sample stacking is not fully
random but instead contains about 4% monoclinic order. Furthermore,
it is shown that the ordered sample has a series of higher-order superstructure
peaks associated with 6-, 9-, 12-, and 15-layer periods whose existence
is transiently driven by the presence of long-range strain that is
an inherent consequence of the synthesis mechanism revealed through
the present diffraction and imaging studies. This strain is closely
associated with a monoclinic shear that can be directly calculated
from cell lattice parameters and is strongly correlated with the degree
of ordering in the samples. The present results are broadly applicable
to other honeycomb-lattice systems, including Li<sub>2</sub>MnO<sub>3</sub> and related Li-excess cathode compositions
Feasibility of Using Li<sub>2</sub>MoO<sub>3</sub> in Constructing Li-Rich High Energy Density Cathode Materials
Layer-structured <i>x</i>Li<sub>2</sub>MnO<sub>3</sub>·(1 – <i>x</i>)ÂLi<i><b>M</b></i>O<sub>2</sub> are promising cathode
materials for high energy-density
Li-ion batteries because they deliver high capacities due to the stabilizing
effect of Li<sub>2</sub>MnO<sub>3</sub>. However, the inherent disadvantages
of Li<sub>2</sub>MnO<sub>3</sub> make these materials suffer from
drawbacks such as fast energy-density decay, poor rate performance
and safety hazard. In this paper, we propose to replace Li<sub>2</sub>MnO<sub>3</sub> with Li<sub>2</sub>MoO<sub>3</sub> for constructing
novel Li-rich cathode materials and evaluate its feasibility. Comprehensive
studies by X-ray diffraction, X-ray absorption spectroscopy, and spherical-aberration-corrected
scanning transmission electron microscopy clarify its lithium extraction/insertion
mechanism and shows that the Mo<sup>4+</sup>/Mo<sup>6+</sup> redox
couple in Li<sub>2</sub>MoO<sub>3</sub> can accomplish the task of
charge compensation upon Li removal. Other properties of Li<sub>2</sub>MoO<sub>3</sub> such as the nearly reversible Mo-ion migration to/from
the Li vacancies, absence of oxygen evolution, and reversible phase
transition during initial (de)Âlithiation indicate that Li<sub>2</sub>MoO<sub>3</sub> meets the requirements to an ideal replacement of
Li<sub>2</sub>MnO<sub>3</sub> in constructing Li<sub>2</sub>MoO<sub>3</sub>-based Li-rich cathode materials with superior performances
A Size-Dependent Sodium Storage Mechanism in Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> Investigated by a Novel Characterization Technique Combining in Situ X‑ray Diffraction and Chemical Sodiation
A novel characterization technique
using the combination of chemical
sodiation and synchrotron based in situ X-ray diffraction (XRD) has
been detailed illustrated. The power of this novel technique was demonstrated
in elucidating the structure evolution of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> upon sodium insertion. The sodium insertion behavior
into Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> is strongly size dependent.
A solid solution reaction behavior in a wide range has been revealed
during sodium insertion into the nanosized Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> (∼44 nm), which is quite different from the
well-known two-phase reaction of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>/Li<sub>7</sub>Ti<sub>5</sub>O<sub>12</sub> system during
lithium insertion, and also has not been fully addressed in the literature
so far. On the basis of this in situ experiment, the apparent Na<sup>+</sup> ion diffusion coefficient (D<sub>Na+</sub>) of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> was estimated in the magnitude of 10<sup>–16</sup> cm<sup>2</sup> s<sup>–1</sup>, close to the
values estimated by electrochemical method, but 5 order of magnitudes
smaller than the Li<sup>+</sup> ion diffusion coefficient (D<sub>Li+</sub> ∼10<sup>–11</sup> cm<sup>2</sup> s<sup>–1</sup>), indicating a sluggish Na<sup>+</sup> ion diffusion kinetics in
Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> comparing with that of
Li<sup>+</sup> ion. Nanosizing the Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> will be critical to make it a suitable anode material for
sodium-ion batteries. The application of this novel in situ chemical
sodiation method reported in this work provides a facile way and a
new opportunity for in situ structure investigations of various sodium-ion
battery materials and other systems
Quantification of Honeycomb Number-Type Stacking Faults: Application to Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> Cathodes for Na-Ion Batteries
Ordered and disordered samples of
honeycomb-lattice Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> were
investigated as cathodes for Na-ion batteries, and it was determined
that the ordered sample exhibits better electrochemical performance,
with a specific capacity of 104 mA h/g delivered at plateaus of 3.5
and 3.2 V (vs Na<sup>+</sup>/Na) with minimal capacity fade during
extended cycling. Advanced imaging and diffraction investigations
showed that the primary difference between the ordered and disordered
samples is the amount of number-type stacking faults associated with
the three possible centering choices for each honeycomb layer. A labeling
scheme for assigning the number position of honeycomb layers is described,
and it is shown that the translational shift vectors between layers
provide the simplest method for classifying different repeat patterns.
It is demonstrated that the number position of honeycomb layers can
be directly determined in high-angle annular dark-field scanning transmission
electron microscopy (STEM-HAADF) imaging studies. By the use of fault
models derived from STEM studies, it is shown that both the sharp,
symmetric subcell peaks and the broad, asymmetric superstructure peaks
in powder diffraction patterns can be quantitatively modeled. About
20% of the layers in the ordered monoclinic sample are faulted in
a nonrandom manner, while the disordered sample stacking is not fully
random but instead contains about 4% monoclinic order. Furthermore,
it is shown that the ordered sample has a series of higher-order superstructure
peaks associated with 6-, 9-, 12-, and 15-layer periods whose existence
is transiently driven by the presence of long-range strain that is
an inherent consequence of the synthesis mechanism revealed through
the present diffraction and imaging studies. This strain is closely
associated with a monoclinic shear that can be directly calculated
from cell lattice parameters and is strongly correlated with the degree
of ordering in the samples. The present results are broadly applicable
to other honeycomb-lattice systems, including Li<sub>2</sub>MnO<sub>3</sub> and related Li-excess cathode compositions
Explore the Effects of Microstructural Defects on Voltage Fade of Li- and Mn-Rich Cathodes
Li-
and Mn-rich (LMR) cathode materials have been considered as promising
candidates for energy storage applications due to high energy density.
However, these materials suffer from a serious problem of voltage
fade. Oxygen loss and the layered-to-spinel phase transition are two
major contributors of such voltage fade. In this paper, using a combination
of X-ray diffraction (XRD), pair distribution function (PDF), X-ray
absorption (XAS) techniques, and aberration-corrected scanning transmission
electron microscopy (STEM), we studied the effects of micro structural
defects, especially the grain boundaries, on the oxygen loss and layered-to-spinel
phase transition through prelithiation of a model compound Li<sub>2</sub>Ru<sub>0.5</sub>Mn<sub>0.5</sub>O<sub>3</sub>. It is found
that the nanosized micro structural defects, especially the large
amount of grain boundaries created by the prelithiation can greatly
accelerate the oxygen loss and voltage fade. Defects (such as nanosized
grain boundaries) and oxygen release form a positive feedback loop,
promote each other during cycling, and accelerate the two major voltage
fade contributors: the transition metal reduction and layered-to-spinel
phase transition. These results clearly demonstrate the important
relationships among the oxygen loss, microstructural defects and voltage
fade. The importance of maintaining good crystallinity and protecting
the surface of LMR material are also suggested
Role of Surface Structure on Li-Ion Energy Storage Capacity of Two-Dimensional Transition-Metal Carbides
A combination of density functional
theory (DFT) calculations and
experiments is used to shed light on the relation between surface
structure and Li-ion storage capacities of the following functionalized
two-dimensional (2D) transition-metal carbides or MXenes: Sc<sub>2</sub>C, Ti<sub>2</sub>C, Ti<sub>3</sub>C<sub>2</sub>, V<sub>2</sub>C,
Cr<sub>2</sub>C, and Nb<sub>2</sub>C. The Li-ion storage capacities
are found to strongly depend on the nature of the surface functional
groups, with O groups exhibiting the highest theoretical Li-ion storage
capacities. MXene surfaces can be initially covered with OH groups,
removable by high-temperature treatment or by reactions in the first
lithiation cycle. This was verified by annealing f-Nb<sub>2</sub>C
and f-Ti<sub>3</sub>C<sub>2</sub> at 673 and 773 K in vacuum for 40
h and <i>in situ</i> X-ray adsorption spectroscopy (XAS)
and Li capacity measurements for the first lithiation/delithiation
cycle of f-Ti<sub>3</sub>C<sub>2</sub>. The high-temperature removal
of water and OH was confirmed using X-ray diffraction and inelastic
neutron scattering. The voltage profile and X-ray adsorption near
edge structure of f-Ti<sub>3</sub>C<sub>2</sub> revealed surface reactions
in the first lithiation cycle. Moreover, lithiated oxygen terminated
MXenes surfaces are able to adsorb additional Li beyond a monolayer,
providing a mechanism to substantially increase capacity, as observed
mainly in delaminated MXenes and confirmed by DFT calculations and
XAS. The calculated Li diffusion barriers are low, indicative of the
measured high-rate performance. We predict the not yet synthesized
Cr<sub>2</sub>C to possess high Li capacity due to the low activation
energy of water formation at high temperature, while the not yet synthesized
Sc<sub>2</sub>C is predicted to potentially display low Li capacity
due to higher reaction barriers for OH removal