10 research outputs found
Investigating Local Degradation and Thermal Stability of Charged Nickel-Based Cathode Materials through Real-Time Electron Microscopy
In this work, we take advantage of
in situ transmission electron microscopy (TEM) to investigate thermally
induced decomposition of the surface of Li<sub><i>x</i></sub>Ni<sub>0.8</sub>Co<sub>0.15</sub>Al<sub>0.05</sub>O<sub>2</sub> (NCA)
cathode materials that have been subjected to different states of
charge (SOC). While uncharged NCA is stable up to 400 °C, significant
changes occur in charged NCA with increasing temperature. These include
the development of surface porosity and changes in the oxygen K-edge
electron energy loss spectra, with pre-edge peaks shifting to higher
energy losses. These changes are closely related to O<sub>2</sub> gas
released from the structure, as well as to phase changes of NCA from
the layered structure to the disordered spinel structure, and finally
to the rock-salt structure. Although the temperatures where these
changes initiate depend strongly on the state of charge, there also
exist significant variations among particles with the same state of
charge. Notably, when NCA is charged to <i>x</i> = 0.33
(the charge state that is the practical upper limit voltage in most
applications), the surfaces of some particles undergo morphological
and oxygen K-edge changes even at temperatures below 100 °C,
a temperature that electronic devices containing lithium ion batteries
(LIB) can possibly see during normal operation. Those particles that
experience these changes are likely to be extremely unstable and may
trigger thermal runaway at much lower temperatures than would be usually
expected. These results demonstrate that in situ heating experiments
are a unique tool not only to study the general thermal behavior of
cathode materials but also to explore particle-to-particle variations,
which are sometimes of critical importance in understanding the performance
of the overall system
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
Using Real-Time Electron Microscopy To Explore the Effects of Transition-Metal Composition on the Local Thermal Stability in Charged Li<sub><i>x</i></sub>Ni<sub><i>y</i></sub>Mn<sub><i>z</i></sub>Co<sub>1–<i>y</i>–<i>z</i></sub>O<sub>2</sub> Cathode Materials
In this work, we use <i>in situ</i> transmission electron
microscopy (TEM) to investigate the thermal decomposition that occurs
at the surface of charged Li<sub><i>x</i></sub>Ni<sub><i>y</i></sub>Mn<sub><i>z</i></sub>Co<sub>1–<i>y</i>–<i>z</i></sub>O<sub>2</sub> (NMC) cathode
materials of different composition (with <i>y</i>, <i>z</i> = 0.8, 0.1, and 0.6, 0.2, and 0.4,and 0.3), after they
have been charged to their practical upper limit voltage (4.3 V).
By heating these materials inside the TEM, we are able to directly
characterize near surface changes in both their electronic structure
(using electron energy loss spectroscopy) and crystal structure and
morphology (using electron diffraction and bright-field imaging).
The most Ni-rich material (<i>y</i>, <i>z</i> =
0.8, 0.1) is found to be thermally unstable at significantly lower
temperatures than the other compositionsî—¸this is manifested
by changes in both the electronic structure and the onset of phase
transitions at temperatures as low as 100 °C. Electron energy
loss spectroscopy indicates that (i) the thermally induced reduction
of Ni ions drives these changes, and (ii) this is exacerbated by the
presence of an additional redox reaction that occurs at 4.2 V in the <i>y</i>, <i>z</i> = 0.8, 0.1 material. Exploration of
individual particles shows that there are substantial variations in
the onset temperatures and overall extent of these changes. Of the
compositions studied, the composition of <i>y</i>, <i>z</i> = 0.6, 0.2 has the optimal combination of high energy
density and reasonable thermal stability. The observations herein
demonstrate that real-time electron microscopy provide direct insight
into the changes that occur in cathode materials with temperature,
allowing optimization of different alloy concentrations to maximize
overall performance
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
Structural Changes in Reduced Graphene Oxide upon MnO<sub>2</sub> Deposition by the Redox Reaction between Carbon and Permanganate Ions
We explore structural changes of
the carbon in MnO<sub>2</sub>/reduced
graphene oxide (RGO) hybrid materials prepared by the direct redox
reaction between carbon and permanganate ions (MnO<sub>4</sub><sup>–</sup>) to reach better understanding for the effects of
carbon corrosion on carbon loss and its bonding nature during the
hybrid material synthesis. In particular, we carried out near-edge
X-ray absorption fine structure spectroscopy at the C K-edge (284.2
eV) to show the changes in the electronic structure of RGO. Significantly,
the redox reaction between carbon and MnO<sub>4</sub><sup>–</sup> causes both quantitative carbon loss and electronic structural changes
upon MnO<sub>2</sub> deposition. Such disruptions of carbon bonding
have a detrimental effect on the initial electrical properties of
the RGO and thus lead to a significant decrease in electrical conductivity.
Electrochemical measurements of the MnO<sub>2</sub>/reduced graphene
oxide hybrid materials using a cavity microelectrode revealed unfavorable
electrochemical properties that were mainly due to the poor electrical
conductivity of the hybrid materials. The results of this study should
serve as a useful guide to rationally approaching the syntheses of
metal/RGO and metal oxide/RGO hybrid materials
Correlating Structural Changes and Gas Evolution during the Thermal Decomposition of Charged Li<sub><i>x</i></sub>Ni<sub>0.8</sub>Co<sub>0.15</sub>Al<sub>0.05</sub>O<sub>2</sub> Cathode Materials
In this work, we present results from the application
of a new
in situ technique that combines time-resolved synchrotron X-ray diffraction
and mass spectroscopy. We exploit this approach to provide direct
correlation between structural changes and the evolution of gas that
occurs during the thermal decomposition of (over)Âcharged cathode materials
used in lithium-ion batteries. Results from charged Li<sub><i>x</i></sub>Ni<sub>0.8</sub>Co<sub>0.15</sub>Al<sub>0.05</sub>O<sub>2</sub> cathode materials indicate that the evolution of both
O<sub>2</sub> and CO<sub>2</sub> gases are strongly related to phase
transitions that occur during thermal decomposition, specifically
from the layered structure (space group <i>R</i>3Ì…<i>m</i>) to the disordered spinel structure (<i>Fd</i>3Ì…<i>m</i>), and finally to the rock-salt structure
(<i>Fm</i>3Ì…<i>m</i>). The state of charge
also significantly affects both the structural changes and the evolution
of oxygen as the temperature increases: the more extensive the charge,
the lower the temperature of the phase transitions and the larger
the oxygen release. Ex situ X-ray absorption spectroscopy (XAS) and
in situ transmission electron microscopy (TEM) are also utilized to
investigate the local structural and valence state changes in Ni and
Co ions, and to characterize microscopic morphology changes. The combination
of these advanced tools provides a unique approach to study fundamental
aspects of the dynamic physical and chemical changes that occur during
thermal decomposition of charged cathode materials in a systematic
way
Structural Changes and Thermal Stability of Charged LiNi<sub><i>x</i></sub>Mn<sub><i>y</i></sub>Co<sub><i>z</i></sub>O<sub>2</sub> Cathode Materials Studied by Combined <i>In Situ</i> Time-Resolved XRD and Mass Spectroscopy
Thermal stability of charged LiNi<sub><i>x</i></sub>Mn<sub><i>y</i></sub>Co<sub><i>z</i></sub>O<sub>2</sub> (NMC, with <i>x</i> + <i>y</i> + <i>z</i> = 1, <i>x</i>:<i>y</i>:<i>z</i> =
4:3:3 (NMC433), 5:3:2 (NMC532), 6:2:2 (NMC622), and 8:1:1 (NMC811))
cathode materials is systematically studied using combined <i>in situ</i> time-resolved X-ray diffraction and mass spectroscopy
(TR-XRD/MS) techniques upon heating up to 600 °C. The TR-XRD/MS
results indicate that the content of Ni, Co, and Mn significantly
affects both the structural changes and the oxygen release features
during heating: the more Ni and less Co and Mn, the lower the onset
temperature of the phase transition (i.e., thermal decomposition)
and the larger amount of oxygen release. Interestingly, the NMC532
seems to be the optimized composition to maintain a reasonably good
thermal stability, comparable to the low-nickel-content materials
(e.g., NMC333 and NMC433), while having a high capacity close to the
high-nickel-content materials (e.g., NMC811 and NMC622). The origin
of the thermal decomposition of NMC cathode materials was elucidated
by the changes in the oxidation states of each transition metal (TM)
cations (i.e., Ni, Co, and Mn) and their site preferences during thermal
decomposition. It is revealed that Mn ions mainly occupy the 3<i>a</i> octahedral sites of a layered structure (<i>R</i>3Ì…<i>m</i>) but Co ions prefer to migrate to the
8<i>a</i> tetrahedral sites of a spinel structure (<i>Fd</i>3Ì…<i>m</i>) during the thermal decomposition.
Such element-dependent cation migration plays a very important role
in the thermal stability of NMC cathode materials. The reasonably
good thermal stability and high capacity characteristics of the NMC532
composition is originated from the well-balanced ratio of nickel content
to manganese and cobalt contents. This systematic study provides insight
into the rational design of NMC-based cathode materials with a desired
balance between thermal stability and high energy density