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Atomistic Simulation Studies of the Electrochemical Activity in Nanocrystalline Li2MnO3

Wednesday, 27 May 2015
Salon C (Hilton Chicago)
P. E. Ngoepe (University of Limpopo, Sovenga, 0727, South Africa), T. X. T. Sayle (University of Kent, Canterbury, CT2 7NZ, UK.), and D. C. Sayle (University of Kent, Canterbury, CT2 7NZ, UK)
Layered-layered oxide composite cathodes, typically of composition xLi2MnO3·(1−x)LiMO2, have attracted much attention, for essentially doubling the capacity available in the earlier generation of Li-ion batteries based on LiCoO2 [1].  However, their use is currently limited by, amongst others, voltage fade [2]. Hence, further studies on one of the end members of the composites, Li2MnO3, could shed valuable insights on such problems.

Li2MnO3 is known to be electrochemically inactive in the parent bulk form and can be rendered Li-active by leaching Li or Li2O from the structure; these Li-deficient compounds are reported to have high intercalation capacities and good reversibility [3]. Alternatively, when synthesized in a nanocrystalline form, Li2MnO3 has been shown to be electrochemically active, yielding capacities up to 200 mAh/g, and excellent capacity retention over multiple cycles [4].

In the current study simulated amorphisation recrystallisation method [5] is used to nucleate and crystallise ternary nanoparticle of Li2MnO3. Simulations of the charging of Li2MnO3 reveal that the reason nanocrystalline- Li2MnO3 is electrochemically active, in contrast to the parent bulk- Li2MnO3, is because in the nanomaterial the alternating Li planes are held apart by Mn ions, which act as a pseudo ‘point defect scaffold’. The Li ions are then able to diffuse, via a vacancy driven mechanism, throughout the nanomaterial in all spatial dimensions while the ‘Mn defect scaffold’ maintains the structural integrity of the layered structure during charging. Our findings reveal that oxides, which comprise cation disorder, can be potential candidates for electrodes in rechargeable Li-ion batteries.

References

[1] Thackeray, M.M., Johnson, C.S., Vaughey, J.T. Li, N. and Hackney, S.A., J. Mater. Chem. 15, 2257, 2005.

[2] Croy J.R., Gallagher K.G., Balasubramanian M., Long B.R. and Thackeray M.M., J. Electrochem. Soc. 161, A318, 2014.

[3] Thackeray M. M. Progr. Solid State Chem. 25, 1, 1997.

[4] Jain, G.R., Yang, J.S., Balasubramanian, M. and Xu, J.J., Chem. Mater. 17, 3850, 2005.      

[5] P.E.Ngoepe, R.R. Maphanga and D.C. Sayle, (2013), “Towards the Nanoscale”, Chapter 9 in Computational Approaches to Energy Materials, pp 261-290, edited by C.R.A. Catlow, A. Sokol and A. Welsch, John Wiley and Sons Ltd.