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Lithium ion batteries for consumer electronics presently command an $11 billion market worldwide (http://www.marketresearch.com/David-Company-v3832/Lithium-Ion-Batteries-Outlook-Alternative-6842261/) and are the premier choice for emerging vehicular applications such as plug-in hybrid electric vehicles (PHEVs) and electric vehicles (EVs). Analogs to these devices utilizing sodium ions rather than lithium are in earlier stages of development, but are considered attractive for large scale energy storage (i.e. grid applications) based on cost and supply security arguments1, 2. Both dual intercalation systems work on the same principle; alkali metal ions shuttle between two electrodes acting as host structures, which undergo insertion processes at different potentials. The electrochemical cells themselves are relatively simple, consisting of composite positive and negative electrodes on current collectors, separated by a porous membrane saturated with an electrolytic solution usually consisting of a salt dissolved in a mixture of organic solvents (Figure 1). Graphite and LiCoO2 are the most commonly employed negative and positive electrodes, respectively, for lithium ion batteries. Several alternative electrode materials have also been developed for specific applications, including variants of LiMn2O4 spinel, LiFePO4 with the olivine structure, and NMCs (LiNixMnxCo1-2xO2 compounds) for positives, and hard carbons, Li4Ti5O12, and alloys of lithium with tin for negatives3. High voltage materials like LiNi0.5Mn1.5O4, new high capacity materials such as layered-layered composites (e.g. xLi2MnO3·(1-x)LiMn0.5Ni0.5O2), compounds with transition metals that can undergo multiple changes in redox states, and Li-Si alloy anodes are currently subjects of intense research, and, if successfully deployed, should raise practical energy densities of lithium ion cells further. Another class of materials, known as conversion electrodes, in which transition metal oxides, sulfides, or fluorides are reversibly reduced to the metallic element and a lithium salt, are also under consideration for use as battery electrodes (primarily as replacements for anodes)4. For devices based on sodium, hard carbons, alloys, NASICON structures, and titanates are being investigated for use as anodes and various transition metal oxides and polyanionic compounds as cathodes.
Because lithium ion and sodium ion batteries are not based on fixed chemistries, their performance characteristics vary considerably depending on the electrodes that are employed. The redox behavior of the electrodes determines the potential profiles, rate capabilities, and cycle lives of the devices. Conventional powder X-ray diffraction (XRD) techniques can be used for initial structural characterization of pristine materials and ex situ measurements on cycled electrodes, but practical considerations such as low signal strength and the relatively long times needed to collect data limit the amount of information that can be obtained on the discharge and charge processes. In contrast, the high brilliance and short wavelengths of synchrotron radiation (e.g. λ=0.97 Å at the Stanford Synchrotron Radiation Lightsource's beamline 11-3), combined with the use of high throughput image detectors, permit acquisition of high-resolution data on samples in as little as 10 sec. In situ work is performed in transmission mode on cell components undergoing charge and discharge in hermetically sealed pouches transparent to X-rays, without having to stop operation to acquire data. As a result, electrode structural changes can be observed as "snapshots in time" as the cell cycles, and much more information can be obtained than with conventional techniques.
X-ray absorption spectroscopy (XAS), also sometimes referred to as X-ray Absorption Fine Structure (XAFS) gives information about the local electronic and geometric structure of materials. In XAS experiments, the photon energy is tuned to the characteristic absorption edges of the specific elements under investigation. Most commonly for battery materials, these energies correspond to the K-edges (1s orbitals) of the transition metals of interest, but soft XAS experiments tuned to O, F, C, B, N and the L2,3 edges of first row transition metals are also sometimes carried out on ex situ samples5. The spectra generated by XAS experiments can be divided into several distinct regions, containing different information (see Newville, M., Fundamentals of XAFS, http://xafs.org/Tutorials?action=AttachFile&do=get&target=Newville_xas_fundamentals.pdf). The main feature, consisting of the absorption edge and extending about 30-50 eV beyond is the X-ray Absorption Near Edge Structure (XANES) region and indicates the ionization threshold to continuum states. This contains information about the oxidation state and coordination chemistry of the absorber. The higher energy portion of the spectrum is known as the Extended X-ray Absorption Fine Structure (EXAFS) region and corresponds to the scattering of the ejected photoelectron off neighboring atoms. Fourier analysis of this region gives short-range structural information such as bond lengths and the numbers and types of neighboring ions. Preedge features below the characteristic absorption energies of some compounds also sometimes appear. These arise from dipole forbidden electronic transitions to empty bound states for octahedral geometries, or dipole allowed orbital hybridization effects in tetrahedral ones and can often be correlated to the local symmetry of the absorbing ion (e.g. whether it is tetrahedrally or octahedrally coordinated)6.
XAS is a particularly useful technique for studying mixed metal systems such as NMCs to determine initial redox states and which transition metal ions undergo redox during delithiation and lithiation processes. Data on several different metals can be obtained rapidly in a single experiment and interpretation is reasonably straightforward. In contrast, Mossbauer spectroscopy is limited to only a few metals used in battery materials (primarily, Fe and Sn). While magnetic measurements can also be used to determine oxidation states, magnetic coupling effects can complicate interpretation particularly for complex oxides such as the NMCs.
Well-planned and -executed in situ and ex situ synchrotron XRD and XAS experiments give complementary information and allow a more complete picture to be formed of the structural changes occurring in electrode materials during normal battery operation than what can be obtained via conventional techniques. This, in turn, gives a greater understanding of what governs the electrochemical behavior of the devices.