Zezhou Guo’s research while affiliated with University of Texas at Austin and other places

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Publications (7)


a) Evolution of total surface residual Li, Li2CO3, and surface LiOH contents in fresh (cathode‐F) and aged cathodes after different air‐storage periods (measured monthly), which are named as cathode‐A‐1 M, cathode‐A‐2 M, cathode‐A‐3 M, respectively. b) Normalized ToF‐SIMS depth profiles and c) difference in the normalized depth profiles of ⁶²NiO– and ⁶²Ni– fragments in LNO, NC, NM, and NA cathodes after three months of air‐storage. d) TEM images of the aged LNO cathode before and after high‐energy electron beam showering. e) Schematic illustration of the architecture of surface degradation products on LNO‐based cathodes after three months of air‐storage. The titration experiment was repeated two times for each sample at each condition for reliability and the average value is presented.
a) Schematic illustration of an experimental setup to control the temperature for the reaction between the cathode and water. b) Reactions between cathode and water and equations for calculating imagined LiOH concentration ([LiOH]IM), reaction rate constant, and activation energy. c) [LiOH]IM‐reaction time plot and the schematic illustration of reactions between cathode particles and water. d) [LiOH]IM‐reaction time plot of LNO cathode at various temperatures. e) lnk‐1/T plot of reactions between LNO and water. f) activation energy for the reactions between the four cathodes and water. The titration experiment was repeated two times for each sample at each condition for reliability and the average value is presented.
a) Schematic illustration of the re‐calcination treatment for aged cathodes and the total surface residual Li contents of fresh, aged (three months of air storage), and re‐calcined (cathode‐R) LNO, NC, NM, and NA cathodes. b) XPS O 1s spectra of fresh, aged, and re‐calcined LNO and NM cathodes. c) Cycling performance and d) EIS plots of fresh, aged, and re‐calcined LNO, NC, NM, and NA. The cells were cycled at a C/3 rate between 2.8 and 4.4 V. 1 C = 180 mA g⁻¹. The electrochemical performance data are based on the average of three or four parallel cells.
In situ XRD contour plots of (003) diffraction peaks of a) fresh and aged LNO and b) fresh and aged NM cathodes during charge. c) Evolution of the c lattice parameter of fresh and aged LNO and NM cathodes during charge. d) Schematic illustration of the delithiated states of cathode primary particles in fresh and aged cathodes when charged to different SOCs.
Selected area electron diffraction and STEM images of a) LNO‐A, b) NM‐A, c) LNO‐R, and d) NM‐R. e) O K‐edge, Ni L‐edge, and Mn L‐edge EELS plots of the layered (orange) and spinel‐like (blue) phases in the NM‐A cathode. Two locations were tested for each region. f) Octahedral crystal field stabilization energy, tetrahedral crystal field stabilization energy, and octahedral‐site stabilization energy for Mn⁴⁺, Mn³⁺, Ni³⁺, and Ni²⁺ cations. g) Schematic illustration of the surface lattice reconstruction pathways of LNO and Mn‐doped NM cathodes.
Formation and Detriments of Residual Alkaline Compounds on High‐Nickel Layered Oxide Cathodes
  • Article
  • Publisher preview available

June 2024

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33 Reads

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6 Citations

Zehao Cui

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Zezhou Guo

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Arumugam Manthiram

High‐nickel layered oxides LiNixM1‐xO2 (x ≥ 0.9) have emerged as promising cathode materials for automotive batteries due to their high energy density and lower cost. However, the formation and accumulation of surface alkaline compounds during storage hinder their mass production and commercialization. Here, a validated chemical method is employed to deconvolute and quantify the evolution of each residual lithium compound in four representative cathodes during ambient‐air storage, viz., LiNiO2 (LNO), LiNi0.95Co0.05O2 (NC), LiNi0.95Mn0.05O2 (NM), and LiNi0.95Al0.05O2 (NA). Furthermore, the activation energy of the reaction between water and the cathode is determined by measuring the leached LiOH concentration at various temperatures. While residual lithium and time‐of‐flight secondary‐ion mass spectrometry measurements collectively reveal that the air stability overall follows the trend of NM > NA ≈ NC > LNO, the aged NM exhibits the highest charge‐transfer resistance and the worst electrochemical performance among the cathodes. In situ, X‐ray diffraction and scanning transmission electron microscopy unveil that the aged NM is plagued by a large area of resistive spinel‐like M3–xLixO4 phases, leading to aggravated particle reaction heterogeneity. Finally, a one‐step recalcination method is demonstrated effective in fully restoring the degraded cathodes. This work provides insights into overcoming air sensitivity issues of high‐Ni cathodes.

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(a) XRD pattern and SEM image of NMC811 cathode. Schematic illustration of the (b) T pulse and (c) pouch cells. (d) Cycling performance of Gr|NMC811 pouch cells with and without the T pulse. (e) Charge‐discharge curves of pouch cells during the T pulse. (f) Electrochemical impedance spectroscopy data of pouch cells. (g) Charge‐discharge curves of post‐mortem half‐cells with cycled cathodes and fresh Li‐metal anodes.
(a) Normalized TOF‐SIMS depth profiles of cathode electrodes with and without the T pulse (after 200 cycles). (b) Illustration of region‐of‐interest (ROI) analyses on the cathode electrodes. ROI‐1 and ROI‐2 represent active material (⁶⁰Ni⁻) and carbon black (C5⁻) domains, respectively. (c) TOF‐SIMS spectra of cathode electrodes based on ROI‐1 and ROI‐2 domains.
(a) Normalized TOF‐SIMS depth profiles of cathode electrodes with and without T pulse after 800 cycles. (b) Intensity of several secondary‐ion fragments sputtered from cycled cathode electrodes. (c) 3D rendering of PO2⁻, C2HO⁻, and ⁶⁰Ni⁻ fragments and carpet plot of the ⁶⁰Ni⁻ fragment. (d) XPS C, O, F, and P atomic concentrations of cathode electrodes after 200 and 800 cycles. The sputtered volume is 100 μm (length) ×100 μm (width) ×180 nm (height)
(a) Normalized TOF‐SIMS depth profiles of graphite anodes in pouch cells with and without the T pulse (after 200 cycles). (b) 3D rendering of selected secondary‐ion fragments. The sputtered volume is 100 μm (length) ×100 μm (width) ×20 nm (height).
(a) Normalized TOF‐SIMS depth profiles of graphite anodes in pouch cells with and without the T pulse (after 800 cycles). (b) Evolution of SEI and metallic Li deposit thickness on graphite anode during cycling. (c) Intensity of several secondary‐ion fragments sputtered from cycled graphite electrodes. Top view of 3D rendering images of several secondary‐ion fragments sputtered from graphite electrodes in cells (d) without and (e) with the T pulse. (f) Schematic illustration of the impact of the T pulse on the interphase chemistry in Gr|NMC811 full cells. The sputtered area is 100 μm (length) ×100 μm (width).
Irreparable Interphase Chemistry Degradation Induced by Temperature Pulse in Lithium‐Ion Batteries

November 2023

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112 Reads

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21 Citations

While it is widely recognized that the operating temperature significantly affects the energy density and cycle life of lithium‐ion batteries, the consequence of electrode‐electrolyte interphase chemistry to sudden environmental temperature changes remains inadequately understood. Here, we systematically investigate the effects of a temperature pulse (T pulse) on the electrochemical performance of LiNi0.8Mn0.1Co0.1O2 (NMC811) pouch full cells. By utilizing advanced characterization tools, such as time‐of‐flight secondary‐ion mass spectrometry, we reveal that the T pulse can lead to an irreversible degradation of cathode‐electrolyte interphase chemistry and architecture. Despite negligible immediate impacts on the solid‐electrolyte interphase (SEI) on graphite anode, aggregated cathode‐to‐anode chemical crossover gradually degrades the SEI by catalyzing electrolyte reduction decomposition and inducing metallic dead Li formation because of insufficient cathode passivation after the T pulse. Consequently, pouch cells subjected to the T pulse show an inferior cycle stability to those free of the T pulse. This work unveils the effects of sudden temperature changes on the interphase chemistry and cell performance, emphasizing the importance of a proper temperature management in assessing performance.


Irreparable Interphase Chemistry Degradation Induced by Temperature Pulse in Lithium‐Ion Batteries

November 2023

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11 Reads

Angewandte Chemie

While it is widely recognized that the operating temperature significantly affects the energy density and cycle life of lithium‐ion batteries, the consequence of electrode‐electrolyte interphase chemistry to sudden environmental temperature changes remains inadequately understood. Here, we systematically investigate the effects of a temperature pulse (T pulse) on the electrochemical performance of LiNi0.8Mn0.1Co0.1O2 (NMC 811) pouch full cells. By utilizing advanced characterization tools, such as time‐of‐flight secondary‐ion mass spectrometry, we reveal that the T pulse can lead to an irreversible degradation of cathode‐electrolyte interphase chemistry and architecture. Despite negligible immediate impacts on the solid‐electrolyte interphase (SEI) on graphite anode, aggregated cathode‐to‐anode chemical crossover gradually degrades the SEI by catalyzing electrolyte reduction decomposition and inducing metallic dead Li formation because of insufficient cathode passivation after the T pulse. Consequently, pouch cells subjected to the T pulse show an inferior cycle stability to those free of the T pulse. This work unveils the effects of sudden temperature changes on the interphase chemistry and cell performance, emphasizing the importance of a proper temperature management in assessing performance.


Effect of Oxidative Synthesis Conditions on the Performance of Single‐Crystalline LiMn2‐xMxO4 (M = Al, Fe, and Ni) Spinel Cathodes in Lithium‐Ion Batteries

October 2023

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37 Reads

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9 Citations

LiMn2O4 (LMO) spinel cathode materials attract much interest due to the low price of manganese and high power density for lithium‐ion batteries. However, the LMO cathodes suffer from the Mn dissolution problem at particle surfaces, which accelerates capacity fade. Herein, the authors report that the oxidative synthesis condition is a key factor in the cell performance of single‐crystalline LiMn2‐xMxO4 (0.03 ≤ x ≤ 0.1, M = Al, Fe, and Ni) cathode materials prepared at 1000 °C. The use of oxygen flow during the spinel‐phase formation minimizes the presence of oxygen vacancies generated at 1000 °C, thereby yielding a stoichiometrically doped LMO product; otherwise, the spinel cathode prepared in atmospheric air readily loses capacity due to the oxygen vacancies in the structure. As a way of circumventing the use of oxygen flow, a one‐pot, two‐step heating in air at 1000 °C and subsequently at 600 °C is used to yield the stoichiometric LMO product. The lithiation heating at 1000–600 ⁰C resulted in a significant improvement in the cycling stability of the prepared LMO cathode in graphite‐based full cells. This study on oxidative synthesis conditions also confirms the advantage of minimizing the surface area of the cathode particles.


Localized High‐Concentration Electrolytes with Low‐Cost Diluents Compatible with Both Cobalt‐Free LiNiO2 Cathode and Lithium‐Metal Anode

August 2023

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198 Reads

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35 Citations

High‐nickel layered oxide cathodes and lithium‐metal anode are promising candidates for next‐generation battery systems due to their high energy density. Nevertheless, the instability of the electrode–electrolyte interphase is hindering their practical application. Localized high‐concentration electrolytes (LHCEs) present a promising solution for achieving uniform lithium deposition and a stable cathode–electrolyte interphase. However, the limited choice of diluents and their high cost are restricting their implementation. Four novel cost‐effective diluents and their performance with highly reactive LiNiO2 cathode and Li‐metal anode are reported here. The results show that all the LHCE cells exhibit a Coulombic efficiency of >99.38% in Li | Cu cells and a capacity retention of >85% in Li | LiNiO2 cells after 250 cycles. Advanced characterizations unveil that the stable cell operation is due to well‐tuned electrode–electrolyte interphases and Li deposition morphology. In addition, online electrochemical mass spectroscopy and differential scanning calorimetry reveal that the gas generation and heat‐release are greatly reduced with the LHCEs presented. Overall, the study provides new insights into the role of diluents in LHCEs and offers valuable guidance for further optimization of LHCEs for high energy density lithium‐metal batteries.


Assessing the Intrinsic Roles of Key Dopant Elements in High‐Nickel Layered Oxide Cathodes in Lithium‐Based Batteries

February 2023

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57 Reads

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57 Citations

A rational compositional design is critical for utilizing LiNiO2‐based cathodes with Ni contents > 90% as promising next‐generation cathode materials. Unfortunately, the lack of a fundamental understanding of the intrinsic roles of key elements, such as cobalt, manganese, and aluminum, makes the rational compositional design of high‐Ni cathodes with a limited range of dopants (<10%) particularly challenging. Here, with 5% single‐element doped cathodes, viz., LiNi0.95Co0.05O2, LiNi0.95Mn0.05O2, and LiNi0.95Al0.05O2, along with undoped LiNiO2 (LNO), the influences of the dopants are systematically examined through a control of cutoff charge energy density and a common practice of cutoff charge voltage. Comprehensive investigations into the electrochemical properties, combined with in‐depth analyses of the structural and interfasial stabilities and electrolyte decomposition pathways through advanced characterizations, unveil the following: i) the intrinsic role of dopants regulates the cathode energy density or state‐of‐charge and, more critically, the occurrence of H2–H3 phase transition, which essentially dictates cyclability; ii) undoped LNO can be stabilized well with the avoidance of H2–H3 phase transition; and iii) Co provides more merits overall with an optimized electrochemical operating condition. This work provides guidance for the compositional design of high‐energy‐density high‐Ni cathodes and sheds light on the challenges of removing Co.

Citations (5)


... V (vs Li/Li + ) range. [54,[63][64][65][66][67] Moreover, this study highlights the necessity of scientific understanding of the surface degradation mechanism of the electrode materials, which has remained relatively mysterious compared to the extensively established bulk degradation theories, for developing long-lasting batteries. We believe the complexity of the surface chemistry due to its intrinsic sensitivity to external conditions, such as current density, voltage, temperature, and even pressure has limited the fundamental understanding. ...

Reference:

Reduction‐Induced Oxygen Loss: the Hidden Surface Reconstruction Mechanism of Layered Oxide Cathodes in Lithium‐Ion Batteries
Formation and Detriments of Residual Alkaline Compounds on High‐Nickel Layered Oxide Cathodes

... Above 4.2 V, the H2 phase transforms to H3 which causes an abrupt anisotropic lattice contraction, destabilizing the mechanical integrity of the cathode. [20][21][22] Above 4.3 V, the H3 phase transforms further to the H4 phase as nearly all of the Li ions are removed from the lattice. In the process, the absence of Li + ions in the Van der Waals gaps favors the gliding of the [NiO 2 ] slabs such that the O3 stacking (AB CA BC) of the H3 phase changes to the O1 stacking (AB AB AB) in the H4 phase. ...

Reducing the Initial Capacity Loss in High-Nickel Cathodes with a Higher Upper Cut-off Voltage Formation Cycle Protocol
  • Citing Article
  • June 2024

ACS Energy Letters

... respectively. However, the study did not account for temperature variations during BT operation, a critical factor of degradation [83]. Furthermore, in the decision-making process for the NMC mode selection module, if the SoC of the lithium-ion BTs (SoClib) falls below the SoClib_low limit, the power output from both the BT and the SC is set to zero. ...

Irreparable Interphase Chemistry Degradation Induced by Temperature Pulse in Lithium‐Ion Batteries

... The shielding effect of 4 M NaTFSI/SUL:FEC is much stronger because all TFSI − are well dispersed in the solvent and almost every Na + is shielded and surrounded by multiple TFSI − . However, in 1.2 M NaTFSI/SUL:OTE:FEC, the diluent molecules separated the contact ion pairs (CIPs) and aggregates (AGGs) in the electrolyte so that the TFSI − from different CIPs and AGGs could not interfere with each other, which weakened the shielding effect against Na + [48]. Compared to 1.2 M NaTFSI/SUL:FEC, the 1.2 M NaTFSI/SUL:OTE:FEC peak is displaced toward the upper field, suggesting a stronger interaction of Na + with TFSI − . ...

Localized High‐Concentration Electrolytes with Low‐Cost Diluents Compatible with Both Cobalt‐Free LiNiO2 Cathode and Lithium‐Metal Anode

... The cathode slurries were prepared by mixing the cathode active material, conductive carbon black C65 and poly(vinylidene fluoride) binder in a weight ratio of 90:5:5 in N-methyl-2-pyrrolidone solvent (to give a solid content of ~43%) using a Thinky mixer at 2,000 revolutions per min for 10 min. The well-mixed slurries were cast onto Al foils to achieve an active material loading of ~25 mg cm −2 , before being dried at 120 °C in a vacuum oven for ≥12 h and then punched into electrode discs (12 mm) for the fabrication of coin cells 50 . ...

Assessing the Intrinsic Roles of Key Dopant Elements in High‐Nickel Layered Oxide Cathodes in Lithium‐Based Batteries