Application Note 093 (pdf 2.2 Mb)

Sergey Shashkov, and Pavel Dorozhkin
Quantum Design, Japan
NT-MDT Co., Moscow Russia

INTRODUCTION

Development of advanced lithium batteries currently represents a very rapidly growing field of science and technology. Lithium batteries are interesting as a power source in numerous portable devices such as notebook computers, cellular phones and camcorders, in electrical vehicles, in military and aerospace applications.

Layered lithium cobalt oxide LiCoO₂ (Fig. 1) is the most commonly used cathode material in commercial lithium batteries. This is due to its longer cycle life, lower self-discharge rate and higher energy density compared to other rechargeable batteries (lead-acid, nickel cadmium or nickel metal hydride), higher cost effectiveness and smaller toxicity.

The layered form of LiCoO₂ has a rhombohedral symmetry with the cell parameters a=2.816 Å and c=14.09 Å [1]. Li and Co ions occupy alternate layers in octahedral sites between the close packed oxygen planes (Fig. 1).

LiCoO₂ structures have been extensively investigated, because such layered structures are perfectly suited to accommodate large changes of the Li content and provide the best pathway for Li⁺ diffusion in and out of the lattice of crystal during the charge–discharge processes:

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It means that lithium ions must additionally travel through this new film. It may change the surface electrochemistry and lead to the unconventional charge/discharge chains.

There are also irreversible processes of electrolyte oxidation and reduction. Batteries can be overcharged with such circumstances; the cathode can undergo phase transformations. Microcrystals of Li_1-xCoO₂ (0<x<0.1) exist in the rhombohedral form with the cell parameters a=2.816 Å and c=14.09 Å. A little more de- lithiated Li_1-xCoO₂ (0.45<x<0.57) passes into a monoclinic structure. Upon further lithium extraction Li_1-xCoO₂ (x>0.57) enters the rhombohedrical form region again.

The c-axis of the crystal unit cell is increased from 14.09 Å to 14.26 Å, but the a-axis is decreased a bit (from 2.816 Å to 2.812 Å) at such transformation. As a result, the volume expansion of few percent is observed [1].

Phase transformations can lead to deterioration of electrical performance or even to degradation of cathode due to the mechanical strain, for example.

Significant deformations in CoO₆ octahedrons and formation of Co₃O₄ / Li₂O can disrupt the intercalation / de-intercalation frameworks.

The formation of lithium oxide (Li₂O) inside batteries during prolonged cycling or storing according to the following reaction [2]

3LiCoO₂ + Li⁺ + e^- = Co₃O₄ + 4Li₂O

can not be reversed electrochemically without destroying the battery. The cathode degrades through loss of Li₂O and transforming LiCoO₂ into electrochemically inactive Co₃O₄.

Understanding distribution of degraded areas on the surface of a positive electrode is very important to improve life time of the batteries.

With the current trend of miniaturization and performance improvement, there is a need for knowledge of Li-ion batteries, Li intercalation and cathode degradation, on a sub-micron scale.

EXPERIMENTAL

Raman spectroscopy and atomic force microscopy (AFM) are valuable methods for the structural characterization of materials used as electrodes in rechargeable lithium batteries (LiCoO₂ in particular). In this note, we present results on a LiCoO cathode characterization measured by AFM and Raman techniques on the integrated instrument NTEGRA Spectra (NT-MDT) integrated with Renishaw inVia Raman spectrometer. The instrument allows simultaneous recording of various AFM and Raman images from the same sample area.

Typical structure of lithium-ion rechargeable cylindrical cell is shown on Fig. 2. The three primary functional components of a lithium-ion battery are the anode, cathode, and electrolyte. Carbonaceous material is used as an anode material (the most commercially popular anode material is graphite).

The inorganic compound, LiCoO₂, is used as the cathode material in the cylindrical cell. The electrolyte is a lithium salt in an organic solvent. The soft separators used in batteries must avoid direct contact between the anode and cathode, but they must allow a free transport of the electrolyte and lithium ions. The batteries typically have a nominal voltage around 3.7 volts.

Individual Lithium-ion ICR-18650 cylindrical cells from different laptop Lithium Battery Packs were investigated.

The first battery pack was used for about 3 years, passed about 1200 charging/recharging cycles and had only about 25% of nominal capacity; the battery was ~30% charged. The second battery was new and ~65 % charged.

Cylindrical cells were opened to separate the cathodes. Cathodes were immediately washed with anhydrous tetrahydrofuran and dried through the blotting paper after opening the cell. This procedure removed electrolyte salt from the electrode to prevent its reaction with moisture in air.

RESULTS

The surface morphology of LiCoO₂ cathode analyzed by AFM is presented in Fig. 3. AFM topography (Fig. 3a-b), provides information about size of grains, their shape and orientation. Lattice constants of cathode material are a function of the lithium concentration, x, in Li_1-xCoO₂ as described above. As a result, the surface of the new LiCoO₂ cathode is more smooth [3]; size of grains derived from the AFM topography images is ~2–2.5 µm. The used battery, cathode exhibits high roughness and grain structure; size of grains is ~2.5–3.5 µm. This is typical, due to the lithium extraction (in case of de-lithiated LiCoO₂), the crystal cell of LiCoO₂ is expanded and individual strained microcrystals of the cathode material may be observed on the surface.

Phase and magnitude of cantilever oscillation recorded during scanning provide complementary information to AFM topography. Phase imaging shows a clear contrast once there is a detectable variation of interaction forces between cantilever and surface. Thus, phase images highlight grain edges and are not affected by large-scale height differences providing clearer observation of the sample fine features (Fig. 3c-d). Magnitude (cantilever oscillation amplitude signal) provide additional contrast (Fig. 3e‑f): grain edges are also clearly observed because control electronics does not respond instantaneously to the sharp changes in the sample height.

Optical images give complementary information to the AFM measurements. There is not complete correlation between the optical and AFM images (Fig. 3). Optical images of the cathode are formed by reflected light that is sensitive to the nature of the interface and grain reflection properties. The amount of light reflected back to the video CCD depends on crystal surface orientation.

Raman spectra of the LiCoO₂ cathode depend on the electrochemical history. From different points on the cathode (Fig. 3) different spectra can be observed (Fig. 4).

By factor group analysis, the total irreducible representation for the vibrational modes of LiCoO₂ is obtained as A1g + 2A2u + Eg + 2Eu. The gerade modes are Raman active and the ungerade modes are IR active. Only two bands should be observed in Raman spectra of LiCoO₂: A1g+ Eg. In fact, experimental spectra of LiCoO exhibit two strong bands at 472 cm^-1 and 579 cm^-1 with the intensity ratio of 1:3 (red spectrum on Fig. 4), which correspond to oxygen vibrations involving v2 (Eg), O-Co-O bending, and v1 (A1g), Co-O stretching modes, respectively (Fig. 5). In the A1g mode two oxygen atoms vibrate in the opposite directions parallel to the c-axis of LiCoO₂, while in the Eg mode they vibrate in the opposite directions parallel to the Co atom planes [4] (Fig. 5).

The positions of these peaks and their intensity are very sensitive to the long- range order in CoO₂ slabs.

Upon the extraction of lithium from the cathode (during battery charging process), some changes are observed in the Raman spectra (green spectrum in Fig. 4). The intense peaks of the LiCoO (472 cm^-1 and 579 cm^-1 bands) experience a small spectral shift. Intensity of 515 cm^-1 and 674 cm^-1 bands is increased. The peak centered at 674 cm^-1 (blue spectrum in Fig. 4) may be assigned to a mode vibration of Co₃O₄ species; the peak at 515 cm^-1 may be assigned to a mode vibration of Li₂O.