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. 2017 Feb 1:8:14309.
doi: 10.1038/ncomms14309.

Phase transformation mechanism in lithium manganese nickel oxide revealed by single-crystal hard X-ray microscopy

Affiliations

Phase transformation mechanism in lithium manganese nickel oxide revealed by single-crystal hard X-ray microscopy

Saravanan Kuppan et al. Nat Commun. .

Abstract

Understanding the reaction pathway and kinetics of solid-state phase transformation is critical in designing advanced electrode materials with better performance and stability. Despite the first-order phase transition with a large lattice mismatch between the involved phases, spinel LiMn1.5Ni0.5O4 is capable of fast rate even at large particle size, presenting an enigma yet to be understood. The present study uses advanced two-dimensional and three-dimensional nano-tomography on a series of well-formed LixMn1.5Ni0.5O4 (0≤x≤1) crystals to visualize the mesoscale phase distribution, as a function of Li content at the sub-particle level. Inhomogeneity along with the coexistence of Li-rich and Li-poor phases are broadly observed on partially delithiated crystals, providing direct evidence for a concurrent nucleation and growth process instead of a shrinking-core or a particle-by-particle process. Superior kinetics of (100) facets at the vertices of truncated octahedral particles promote preferential delithiation, whereas the observation of strain-induced cracking suggests mechanical degradation in the material.

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Conflict of interest statement

The authors declare no competing financial interests.

Figures

Figure 1
Figure 1. XANES measurement of the crystal samples.
(a) Experimentally measured Ni K-edge XANES spectra of chemically delithiated LixMn1.5Ni0.5O4 (LixMNO) crystals, (b) Ni edge energy as a function of the state of charge in LixMNO samples, (c) Ni K-edge XANES spectra of phase-pure LiMn1.5Ni0.5O4 (red), Li0.5Mn1.5Ni0.5O4 (green) and Mn1.5Ni0.5O4 (blue) phases. The experimentally measured spectrum of Li0.51Mn1.5Ni0.5O4 (black) is also shown for comparison, d,e enlarged views of the two highlighted regions in c. Horizontal error bars in b were obtained by quantifying the SOC multiple times. Vertical error bars in b were obtained by evaluating the energy resolution of the beamline used for the XANES measurements.
Figure 2
Figure 2. Two-dimensional chemical mapping of LixMn1.5Ni0.5O4 crystals.
(a) x=0.82, (b) x=0.71, (c) x=0.51 and (d) x=0.25. (eh) the variation of local XANES spectrum across each particle. (il) the relative concentration of the three chemical phases, as well as the variation in the local oxidation state of Ni within the same particle. Scale bar, 0.5 μm.
Figure 3
Figure 3. Three-dimensional map of Ni oxidation state at sub-particle scale.
The shape of the particle is presented as the transparent grey surface with the internal oxidation state heterogeneity illustrated using the diagonal slices (ad) surfaces of the 3D Ni oxidation state map (ej). All the panels are colour coded in order to show the state of charge heterogeneity at the sub-particle level in a quantitative manner.
Figure 4
Figure 4. Surface facets of LiMn1.5Ni0.5O4 crystals.
(a) Scanning electron microscopy images showing the truncation at some corners of the crystals and (b) atomic models of the (111) and (100) planes in the ordered spinel with a P4332 space group: green balls (Ni cations), magenta balls (Mn cations) and yellow balls (O anions). Scale bars, 10 and 1 μm in a, left and right, respectively.
Figure 5
Figure 5. Schematics of possible phase transformation mechanisms in LiMn1.5Ni0.5O4.
Figure 6
Figure 6. Particle fracturing in chemically delithaiated LixMn1.5Ni0.5O4 crystals.
(a) 3D surface renderings of two selected Mn1.5Ni0.5O4 crystals (the left one at ∼4 μm and the right one at 2 μm) show the formation of irregularly shaped cracks on the particle surface, (b,c) SEM images of pristine LiMn1.5Ni0.5O4 and delithiated Mn1.5Ni0.5O4 crystals, respectively. Scale bars, 1 μm (ac).

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