On the Elusive Crystallography of Lithium‐Rich Layered Oxides: Novel Structural Models

Author:

Celeste Arcangelo1234ORCID,Tuccillo Mariarosaria14,Menon Ashok S.56,Brant William5,Brandell Daniel5,Pellegrini Vittorio7,Brescia Rosaria3,Silvestri Laura4,Brutti Sergio189

Affiliation:

1. Dipartimento di Chimica Sapienza Università di Roma p. le Aldo Moro 5 Rome 00185 Italy

2. Dipartimento di Chimica e Chimica Industriale Università degli Studi di Genova via Dodecaneso 31 Genoa 16146 Italy

3. Istituto Italiano di Tecnologia Via Morego 30 Genova 16163 Italy

4. Dipartimento di Tecnologie Energetiche e Fonti Rinnovabili ENEA C.R. Casaccia via Anguillarese 301 Rome 00123 Italy

5. Department of Chemistry−Ångström Laboratory Uppsala University Uppsala SE‐751 21 Sweden

6. WMG University of Warwick Coventry CV4 7AL UK

7. BeDimensional Spa via Torrentesecca 3d Genoa 16163 Italy

8. ISC‐CNR OUS Sapienza Via dei Tarquini Rome 00185 Italy

9. GISEL—Centro di Riferimento Nazionale per i Sistemi di Accumulo Elettrochimico di Energia INSTM via G. Giusti Florence 50121 Italy

Abstract

AbstractLithium‐rich layered oxides (LRLOs) are one of the most attractive families among future positive electrode materials for the so‐called fourth generation of lithium‐ion batteries (LIBs). Their electrochemical performance is enabled by the unique ambiguous crystal structure that is still not well understood despite decades of research. In the literature, a clear structural model able to describe their crystallographic features is missing thereby hindering a clear rationalization of the interplay between synthesis, structure, and functional properties. Here, the structure of a specific LRLO, Li1.28Mn0.54Ni0.13Co0.02Al0.03O2, using synchrotron X‐ray diffraction (XRD), neutron diffraction (ND), and High‐Resolution Transmission Electron Microscopy (HR‐TEM), is analyzed. A systematic approach is applied to model diffraction patterns of Li1.28Mn0.54Ni0.13Co0.02Al0.03O2 by using the Rietveld refinement method considering the Rm and C2/m unit cells as the prototype structures. Here, the relative ability of a variety of structural models is compared to match the experimental diffraction pattern evaluating the impact of defects and supercells derived from the Rm structure. To summarize, two possible models able to reconcile the description of experimental data are proposed here for the structure of Li1.28Mn0.54Ni0.13Co0.02Al0.03O2: namely a monoclinic C2/m defective lattice (prototype Li2MnO3) and a monoclinic defective supercell derived from the rhombohedral Rm unit cell (prototype LiCoO2).

Publisher

Wiley

Subject

General Materials Science,General Chemistry

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