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Electronic structure of β-NaxV2O5 (x ≈ 0.33) polycrystalline films: Growth, spectroscopy, and theory

Bo Chen, Jude Laverock, Dave Newby, Ting Yi Su, Kevin E. Smith*, Wei Wu, Linda H. Doerrer, Nicholas F. Quackenbush, Shawn Sallis, Louis F.J. Piper, Daniel A. Fischer, Joseph C. Woicik

*Corresponding author for this work

Research output: Contribution to journalArticle (Academic Journal)peer-review

25 Citations (Scopus)

Abstract

We present a detailed study of the microstructure and electronic structure of β-NaxV2O5 (x ≈ 0.33) polycrystalline films, combining film growth, X-ray spectroscopies, and first-principles calculations. High-quality crystalline and stoichiometric V2O 5 and β-Na0.33V2O5 films were grown by a sol-gel process, spin-coating, and rapid thermal annealing. The V2O5 film, which exhibits a rough surface, is preferentially oriented in the (001) direction perpendicular to the surface, whereas the b-axis of β-Na0.33V2O5 is oriented in the substrate plane. The β-Na0.33V2O 5 film consists of a nested layered structure composed of single-crystalline rods of a few hundred nanometers in diameter and a few micrometers in length. Photoemission and X-ray absorption measurements of β-Na0.33V2O5 confirm the Na incorporation and the presence of mixed V5+ and V4+ species and weakly occupied V 3d states. At the V L-edge, X-ray absorption and resonant inelastic X-ray measurements suggest a larger crystal field for β-Na 0.33V2O5 compared with isoelectronic β-Sr0.17V2O5. We observe the lowest local crystal-field dd* transition at an energy of ∼-1.6 ± 0.1 eV for β-Na0.33V2O5, which is substantially larger than β-Sr0.17V2O5; this large difference is interpreted as arising from the stronger distortions to the VO6 octahedra in β-Na0.33V2O5.

Original languageEnglish
Pages (from-to)1081-1094
Number of pages14
JournalJournal of Physical Chemistry C
Volume118
Issue number2
DOIs
Publication statusPublished - 16 Jan 2014

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