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December 12, 2003 In Situ X-ray Absorption Spectroscopic Study on the LiNi0.5Mn0.5O2 Cathode Material during Electrochemical CyclingW.-S. Yoon1, C.P. Grey2, M. Balasubramanian1, X.-Q. Yang1 and J. McBreen1 Lithium ion batteries consist of a layered-lithium first-row transition metal oxide cathode (positive) and a graphite anode (negative) that can intercalate lithium ions. In the intercalation process, Li+ ions migrate into the empty space between the metal oxide or graphite layers. Oppositely, egress of the Li+ ions is called deintercalation. During the repeated charging and discharging of the battery, called cycling, the lithium ions shuttle between the anode and cathode, electrons flow in the external circuit, and the metal in the cathode undergoes a redox process. In this process, the metal’s oxidation state is changed. In situ x-ray absorption spectroscopy (XAS) was used to study the redox processes in LiNi0.5Mn0.5O2. The results indicate that the redox process occurs on the nickel ions, with the conversion of Ni2+ to Ni3+ occurring first and the Ni3+ to Ni4+ conversion occurring second. The manganese remains Mn4+ during normal battery cycling.
In practice, only 50 percent of the Li+ ions are removed from the LiCoO2 cathodes during the charging process. Removal of more than this severely limits the battery’s cycle life. Fortunately, during charging, the cell voltage has a well-defined positive slope (Figure 1), making it possible to remove only 50 percent of the Li+ ions by simply terminating the charge at 4.2 V. However, this results in the utilization of only half the theoretical charge capacity that could be obtained by completely removing the Li+ ions. Because of the low cathode capacity and the cost of LiCoO2, extensive research is underway to find alternative cathode materials with larger operating capacities and lower costs. LiNi0.5Mn0.5O2 is one of the more promising new materials. It has a lower cost, a higher capacity, and is more resistant to thermal abuse than LiCoO2.
We reported an in situ XAS study of LiNi0.5Mn0.5O2, at the Ni and Mn K-edges, as it was charged and discharged. The XAS study was done in the transmission mode in a two-electrode cell with thin mylar windows. The respective K-edges of Mn and Ni metal are at 6539 eV and 8333 eV. At these energies, the x-ray can eject 1s core electrons and there is a large increase in the x-ray absorption. As the oxidation state of the metals increases, there are less electrons to screen the nucleus and the edge position shifts to higher energies because it becomes more difficult to eject the 1s electrons. By monitoring the edge shifts, we can follow the redox processes on both Mn and Ni.
Figure 1 shows a voltage profile of the cell as it was charged over a 50-hour period to remove all the Li+, while continuously recording XAS spectra. Representative XAS scans are indicated on the plot. Figure 2a shows the Mn K-edge x-ray absorption near-edge structure (XANES) and Figure 2b shows the Ni K-edge XANES. Even though there are changes in the Mn XANES during charging, there is no rigid shift of the Mn XANES to higher energies, indicating that the Mn remains Mn4+ throughout charging. However, the Ni XANES shows a rigid shift, indicating the conversion of the initial Ni2+ to Ni4+. Analysis of the Mn extended x-ray absorption fine structure (EXAFS) shows very few changes in the Mn O first-shell interactions, which supports our conclusion from the XANES analysis that Mn remains Mn4+. The Ni EXAFS shows major changes in the Ni O first-shell interactions, which is consistent with the XANES. All of this clearly indicates that charge compensation, during charging, occurs via the oxidation of Ni2+ to Ni4+. Analysis of the EXAFS indicates that this occurs in two steps: first, from Ni2+ to Ni3+, and then from Ni3+ to Ni4+. BEAMLINE FUNDING PUBLICATION FOR MORE INFORMATION |