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Structural Evolution of Disordered LixV2O5 Bronzes in V2O5 Cathodes for Li-Ion Batteries

  • Christian K. Christensen
  • , Daniel R. Sørensen
  • , Jeanette Hvam
  • , Dorthe B. Ravnsbæk*
  • *Kontaktforfatter

Publikation: Bidrag til tidsskrift › Tidsskriftartikel › Forskning › peer review

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Abstract

Vanadium pentaoxide, V2O5, is an attractive cathode material for Li-ion batteries, which can store up to three Li ion per formula unit. At deep discharge, an irreversible reconstructive phase transition occurs with formation of the disordered ω-LixV2O5 bronze, which, despite the lack of long-range order, exhibits a high reversible capacity (∼310 mAh/g) without regaining the crystallinity upon recharge. Here, we utilize operando powder X-ray diffraction and total scattering (i.e., pair distribution function analysis) to investigate the atomic-scale structures of the deep-discharge phase ω-LixV2O5 (x ∼ 3) and, for the first time, the highly disordered phase β-LixV2O5 (x ∼ 0.3) formed during subsequent Li-extraction. Our studies reveal that the deep discharge ω-Li3V2O5 phase consists of ∼60 Å domains rock salt structure with a local cation ordering on an ∼15 Å length scale. The charged β-LixV2O5 phase only exhibits very short-range ordering (∼10 Å). The phase transition between these phases is structurally reversible and appears unexpectedly to occur via a two-phase transition mechanism.

OriginalsprogEngelsk
TidsskriftChemistry of Materials
Vol/bind31
Udgave nummer2
Sider (fra-til)512-520
ISSN0897-4756
DOI
StatusUdgivet - 2019

Finansiering

We thank the Villum Foundation (Grant VKR023453), the Independent Research Fund Denmark (Grant 4184-00143A), and the Carlsberg Foundation (Grant CF17-0823) for funding this research. We also thank Danscatt for financial support. We are grateful for access to the facilities and resources at the synchrotrons Petra III (beamline P02.1) and the Advanced Photon Source (beamline 11-ID-B). The latter is a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory (under Contract No. DE-AC02-06CH11357). Finally, we would like to thank Dr. Olaf J. Borkiewicz and Dr. Kamila M. Wiaderek at beamline 11-ID-B (APS), and Dr. Jozef Bednarcik at beamline P02.1 (Petra III) for experimental support.

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