If you are using this page, please cite:
H. Eckert, S. Divilov, M. J. Mehl, D. Hicks, A. C. Zettel, M. Esters. X. Campilongo and S. Curtarolo, The AFLOW Library of Crystallographic Prototypes: Part 4. Submitted to Computational Materials Science.
FeLiO$_{2}$ exhibits a wide variety of structures, with the exact structure present depends on thermodynamic effects, preparation methods, and charge/discharge history.
We follow the nomenclature of (Kanno, 1996), where appropriate, with modifications found in (Tabuchi, 1995) and (Abdel-Ghany, 2012). The following list of structures is no doubt incomplete:
$\alpha$–LiFeO$_{2}$ is in the cubic rock salt ($B1$) structure, with lithium and iron randomly placed on the sodium site and oxygen on the chlorine site. It is synthesized at temperatures above 600°C.
$\beta$–LiFeO$_{2}$ (this structure) is a tetragonal distortion of $\alpha$–LiFeO$_{2}$ with the lithium and iron atoms still randomly placed on their sublattice (we denote this site as Fe).
$\beta'$–LiFeO$_{2}$ is monoclinic and transforms to $\gamma$–LiFeO$_{2}$ near room temperature. This is likely the phase (Kanno, 1996) refers to as $\beta$–LiFeO$_{2}$.
$\gamma$–LiFeO$_{2}$ is created by low-temperature synthesis below 500°C and can be considered as an ordered version of $\alpha$–LiFeO$_{2}$, with a doubled unit cell.
o-LiFeO$_{2}$ is orthorhombic, produced by an ion exchange interaction. It is (meta)-stable below 400°C, transforming to $\alpha$–LiFeO$_{2}$ above 600°C.
In $\beta$–LiFeO$_{2}$ the iron and lithium atoms occupy the (1a) Wyckoff position equally (Anderson, 1964). We arbitrarily label these as iron here.
(Anderson, 1964) place this in space group $I4/m$ #87, but the atomic positions are consistent with the higher symmetry $I4/mmm$ #139, so we place it there.
$L'2_{0}$ FeC$_{x}$ and $\beta$–LiFeO$_{2}$ have the same AFLOW prototype label, AB_tI4_139_a_b. They are generated by the same symmetry operations with different sets of parameters (--params) specified in their corresponding CIF files.
J. C. Anderson and M. Schieber, Order-disorder transitions in heat-treated rock-salt Lithium Ferrite, J. Phys. Chem. Solids 25, 961–968 (1964), doi:10.1016/0022-3697(64)90033-2.
R. Kanno, T. Shirane, Y. Kawamoto, Y. Takeda, M. Takano, M. Ohashi, and Y. Yamaguchi, Synthesis, Structure, and Electrochemical Properties of a New Lithium Iron Oxide, LiFeO$_{2}$, with a Corrugated Layer Structure, J. Electrochem. Soc. 143, 2435–2442 (1996), doi:10.1149/1.1837027.
A. E. Abdel-Ghany, A. Mauger, H. Groult, K. Zaghib, and C. M. Julien, Structural properties and electrochemistry of α-LiFeO$_{2}$, J. Power Sources 197, 285–291 (2012), doi:10.1016/j.jpowsour.2011.09.054.
Y. S. Lee, S. Sato, Y. K. Sun, K. Kobayakawa, and Y.Sato, A new type of orthorhombic LiFeO$_{2}$ with advanced battery performance and its structural change during cycling}, J. Power Sources \textbf{119-121, 285–289 (2003), doi:10.1016/S0378-7753(03)00152-6.
M. Tabuchi, K. Ado, H. Sakaebe, C. Masquelier, H. Kageyama, and O. Nakamura, Preparation of AFeO$_{2}$ (A = Li, Na) by hydrothermal method, Solid State Ionics 79, 220–226 (1995), doi:10.1016/0167-2738(95)00065-E.
Found in
M. Barré and M. Catti, Neutron diffraction study of the $\beta$' and $\gamma$ phases of LiFeO$_{2}$, J. Solid State Chem. 182, 2549–2554 (2009), doi:10.1016/j.jssc.2009.06.029.