4 research outputs found

    Structural Phase Transition from Rhombohedral (<i>R</i>3̅<i>m</i>) to Monoclinic (<i>C</i>2/<i>m</i>) Symmetry in Lithium Overstoichiometric Li<sub>1+δ</sub>Co<sub>1−δ</sub>O<sub>2−δ</sub>

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    Stoichiometric lithium cobalt oxide LiCoO<sub>2</sub> is known to exhibit several structural phase transitions with <i>x</i> in Li<sub><i>x</i></sub>CoO<sub>2</sub> at ambient temperature (<i>T</i>); e.g., an initial rhombohedral (<i>R</i>3̅<i>m</i>) phase transforms into a monoclinic (<i>C</i>2/<i>m</i>) phase at <i>x</i> ∼ 0.5. In contrast, lithium overstoichiometric (Li)<sub>3<i>b</i></sub>[Li<sub>δ</sub>Co<sub>1−δ</sub>]<sub>3<i>a</i></sub>O<sub>2−δ</sub> with δ ≥ ∼0.02, where δ is the Li<sup>+</sup> ions at the 3<i>a</i> (Co) site, maintains the <i>R</i>3̅<i>m</i> symmetry until <i>x</i> ∼ 0.5 in Li<sub><i>x</i></sub>(Li<sub>δ</sub>Co<sub>1−δ</sub>)­O<sub>2−δ</sub> at ambient <i>T</i>, and this is the reason why such material has been widely used in commercial lithium ion batteries. We performed X-ray diffraction measurements in the <i>T</i> range between 100 and 300 K for the lithium overstoichiometric Li<sub><i>x</i></sub>(Li<sub>0.02</sub>Co<sub>0.98</sub>)­O<sub>1.98</sub> samples with <i>x</i> = 1, 0.56, and 0.51 to understand the factors that govern the structural changes in Li<sub><i>x</i></sub>(Li<sub>δ</sub>Co<sub>1−δ</sub>)­O<sub>2−δ</sub> with δ ≥ 0. Both <i>x</i> = 0.56 and 0.51 samples exhibit a structural phase transition from the high-<i>T R</i>3̅<i>m</i> phase to the low-<i>T C</i>2/<i>m</i> phase at 250 K (=<i>T</i><sub>s1</sub>). Furthermore, these samples indicate another structural phase transition at 170 K (=<i>T</i><sub>s2</sub>); although their crystal structures still have the <i>C</i>2/<i>m</i> symmetry, the degree of monoclinic distortion starts to decrease below <i>T</i><sub>s2</sub>, associated with a magnetic anomaly and a freezing of the Li<sup>+</sup> ions at the 3<i>b</i> site. Because the two structural phase transitions of <i>T</i><sub>s1</sub> (=330 K) and <i>T</i><sub>s2</sub> (=150 K) are also observed for the stoichiometric Li<sub><i>x</i></sub>CoO<sub>2</sub> compound with <i>x</i> ∼ 0.5, the <i>C</i>2/<i>m</i> phase in Li<sub><i>x</i></sub>(Li<sub>δ</sub>Co<sub>1−δ</sub>)­O<sub>2−δ</sub> is found to appear in the limited <i>x</i> and <i>T</i> ranges. The characteristics and possible origin of <i>T</i><sub>s1</sub> and <i>T</i><sub>s2</sub> for both stoichiometric Li<sub><i>x</i></sub>CoO<sub>2</sub> and lithium overstoichiometric Li<sub><i>x</i></sub>(Li<sub>0.02</sub>Co<sub>0.98</sub>)­O<sub>1.98</sub> samples are discussed
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