28 research outputs found

    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

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    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

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    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

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    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

    No full text
    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

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    Layer-structured <i>x</i>Li<sub>2</sub>MnO<sub>3</sub>·(1 – <i>x</i>)­Li<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)­lithiation 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

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    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

    No full text
    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

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    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

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    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
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