6 research outputs found

    Chromium-Modified Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> with a Synergistic Effect of Bulk Doping, Surface Coating, and Size Reducing

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    Bulk doping, surface coating, and size reducing are three strategies for improving the electrochemical properties of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> (LTO). In this work, chromium (Cr)-modified LTO with a synergistic effect of bulk doping, surface coating, and size reducing is synthesized by a facile sol–gel method. X-ray diffraction (XRD) and Raman analysis prove that Cr dopes into the LTO bulk lattice, which effectively inhibits the generation of TiO<sub>2</sub> impurities. Transmission electron microscopy (TEM) and X-ray photoelectron spectroscopy (XPS) verifies the surface coating of Li<sub>2</sub>CrO<sub>4</sub> on the LTO surface, which decreases impedance of the LTO electrode. More importantly, the size of LTO particles can be significantly reduced from submicroscale to nanoscale as a result of the protection of the Li<sub>2</sub>CrO<sub>4</sub> surface layer and the suppression from Cr atoms on the long-range order in the LTO lattice. As anode material, Li<sub>4‑<i>x</i></sub>Cr<sub>3<i>x</i></sub>Ti<sub>5–2<i>x</i></sub>O<sub>12</sub> (<i>x</i> = 0.1) delivers a reversible capacity of 141 mAh g<sup>–1</sup> at 10 °C, and over 155 mAh g<sup>–1</sup> at 1 °C after 1000 cycles. Therefore, the Cr-modified Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> prepared via a sol–gel method has potential for applications in high-power, long-life lithium-ion batteries

    Operando EPR for Simultaneous Monitoring of Anionic and Cationic Redox Processes in Li-Rich Metal Oxide Cathodes

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    Anionic redox chemistry offers a transformative approach for significantly increasing specific energy capacities of cathodes for rechargeable Li-ion batteries. This study employs operando electron paramagnetic resonance (EPR) to simultaneously monitor the evolution of both transition metal and oxygen redox reactions, as well as their intertwined couplings in Li<sub>2</sub>MnO<sub>3</sub>, Li<sub>1.2</sub>Ni<sub>0.2</sub>Mn<sub>0.6</sub>O<sub>2</sub>, and Li<sub>1.2</sub>Ni<sub>0.13</sub>Mn<sub>0.54</sub>Co<sub>0.13</sub>O<sub>2</sub> cathodes. Reversible O<sup>2–</sup>/O<sub>2</sub><sup><i>n</i>–</sup> redox takes place above 3.0 V, which is clearly distinguished from transition metal redox in the operando EPR on Li<sub>2</sub>MnO<sub>3</sub> cathodes. O<sup>2–</sup>/O<sub>2</sub><sup><i>n</i>–</sup> redox is also observed in Li<sub>1.2</sub>Ni<sub>0.2</sub>Mn<sub>0.6</sub>O<sub>2</sub>, and Li<sub>1.2</sub>Ni<sub>0.13</sub>Mn<sub>0.54</sub>Co<sub>0.13</sub>O<sub>2</sub> cathodes, albeit its overlapping potential ranges with Ni redox. This study further reveals the stabilization of the reversible O redox by Mn and e<sup>–</sup> hole delocalization within the Mn–O complex. The interactions within the cation–anion pairs are essential for preventing O<sub>2</sub><sup><i>n</i>–</sup> from recombination into gaseous O<sub>2</sub> and prove to activate Mn for its increasing participation in redox reactions. Operando EPR helps to establish a fundamental understanding of reversible anionic redox chemistry. The gained insights will support the search for structural factors that promote desirable O redox reactions

    Lithiation and Delithiation Dynamics of Different Li Sites in Li-Rich Battery Cathodes Studied by <i>Operando</i> Nuclear Magnetic Resonance

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    Li in Li-rich cathodes mostly resides at octahedral sites in both Li layers (Li<sub>Li</sub>) and transition metal layers (Li<sub>TM</sub>). Extraction and insertion of Li<sub>Li</sub> and Li<sub>TM</sub> are strongly influenced by surrounding transition metals. pjMATPASS and <i>operando</i> Li nuclear magnetic resonance are combined to achieve both high spectral and temporal resolution for quantitative real time monitoring of lithiation and delithiation at Li<sub>Li</sub> and Li<sub>TM</sub> sites in Li<sub>2</sub>MnO<sub>3</sub>, Li<sub>1.2</sub>Ni<sub>0.2</sub>Mn<sub>0.6</sub>O<sub>2</sub>, and Li<sub>1.2</sub>Ni<sub>0.13</sub>Mn<sub>0.54</sub>Co<sub>0.13</sub>O<sub>2</sub> cathodes. The results have revealed that Li<sub>TM</sub> are preferentially extracted for the first 20% of charge and then Li<sub>Li</sub> and Li<sub>TM</sub> are removed at the same rate. No preferential insertion or extraction of Li<sub>Li</sub> and Li<sub>TM</sub> is observed beyond the first charge. Ni and Co promote faster and more complete removal of Li<sub>TM</sub>. The recovery of the removed Li is <60% for Li<sub>TM</sub> and >80% for Li<sub>Li</sub> upon first discharge. The study sheds light on the activity of Li<sub>Li</sub> and Li<sub>TM</sub> during electrochemical processes as well as their respective contributions to cathode capacity

    Li Distribution Heterogeneity in Solid Electrolyte Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> upon Electrochemical Cycling Probed by <sup>7</sup>Li MRI

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    All-solid-state rechargeable batteries embody the promise for high energy density, increased stability, and improved safety. However, their success is impeded by high resistance for mass and charge transfer at electrode–electrolyte interfaces. Li deficiency has been proposed as a major culprit for interfacial resistance, yet experimental evidence is elusive due to the challenges associated with noninvasively probing the Li distribution in solid electrolytes. In this Letter, three-dimensional <sup>7</sup>Li magnetic resonance imaging (MRI) is employed to examine Li distribution homogeneity in solid electrolyte Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> within symmetric Li/Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub>/Li batteries. <sup>7</sup>Li MRI and the derived histograms reveal Li depletion from the electrode–electrolyte interfaces and increased heterogeneity of Li distribution upon electrochemical cycling. Significant Li loss at interfaces is mitigated via facile modification with a poly­(ethylene oxide)/bis­(trifluoromethane)­sulfonimide Li salt thin film. This study demonstrates a powerful tool for noninvasively monitoring the Li distribution at the interfaces and in the bulk of all-solid-state batteries as well as a convenient strategy for improving interfacial stability

    Li Distribution Heterogeneity in Solid Electrolyte Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> upon Electrochemical Cycling Probed by <sup>7</sup>Li MRI

    No full text
    All-solid-state rechargeable batteries embody the promise for high energy density, increased stability, and improved safety. However, their success is impeded by high resistance for mass and charge transfer at electrode–electrolyte interfaces. Li deficiency has been proposed as a major culprit for interfacial resistance, yet experimental evidence is elusive due to the challenges associated with noninvasively probing the Li distribution in solid electrolytes. In this Letter, three-dimensional <sup>7</sup>Li magnetic resonance imaging (MRI) is employed to examine Li distribution homogeneity in solid electrolyte Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub> within symmetric Li/Li<sub>10</sub>GeP<sub>2</sub>S<sub>12</sub>/Li batteries. <sup>7</sup>Li MRI and the derived histograms reveal Li depletion from the electrode–electrolyte interfaces and increased heterogeneity of Li distribution upon electrochemical cycling. Significant Li loss at interfaces is mitigated via facile modification with a poly­(ethylene oxide)/bis­(trifluoromethane)­sulfonimide Li salt thin film. This study demonstrates a powerful tool for noninvasively monitoring the Li distribution at the interfaces and in the bulk of all-solid-state batteries as well as a convenient strategy for improving interfacial stability

    Ultrathin Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> Nanosheets as Anode Materials for Lithium and Sodium Storage

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    Ultrathin Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> (LTO) nanosheets with ordered microstructures were prepared via a polyether-assisted hydrothermal process. Pluronic P123, a polyether, can impede the growth of Li<sub>2</sub>TiO<sub>3</sub> in the precursor and also act as a structure-directing agent to facilitate the (Li<sub>1.81</sub>H<sub>0.19</sub>)­Ti<sub>2</sub>O<sub>5</sub>·2H<sub>2</sub>O precursor to form the LTO nanosheets with the ordered microstructure. Moreover, the addition of P123 can suppress the stacking of LTO nanosheets during calcining of the precursor, and the thickness of the nanosheets can be controlled to be about 4 nm. The microstructure of the as-prepared ultrathin and ordered nanosheets is helpful for Li<sup>+</sup> or Na<sup>+</sup> diffusion and charge transfer through the particles. Therefore, the ultrathin P123-assisted LTO (P-LTO) nanosheets show a rate capability much higher than that of the LTO sample without P123 in a Li battery with over 130 mAh g<sup>–1</sup> of capacity remaining at the 64C rate. For intercalation of larger size Na<sup>+</sup> ions, the P-LTO still exhibits a capacity of 115 mAh g<sup>–1</sup> at a current rate of 10 C and a capacity retention of 96% after 400 cycles
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