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Calculated O K-edge XAS Spectra of Niobium Oxide Phases using Bethe-Salpeter equation

<p>X-ray absorption spectra (XAS) were calculated for the oxygen K-edge for 20 different phases of Niobium oxides (NbO<sub>x</sub>) using the Bethe-Salpeter equation as implemented within the OCEAN code. Fifteen of the NbO<sub>x</sub>&nbsp;phases are amorphous, in which nine are stoichiometric Nb<sub>2</sub>O<sub>5</sub>, and slightly off-stoichiometric containing a variety of different defects. The other five structures are different crystalline phases (with spacegroup): NbO (Pm3m), NbO<sub>2</sub> (P4<sub>2</sub>/mnm), N-Nb<sub>2</sub>O<sub>5</sub> (C<sub>2</sub>/m), M-Nb<sub>2</sub>O<sub>5</sub> (I4/mmm), and B-Nb<sub>2</sub>O<sub>5</sub> (C<sub>2</sub>/c). The data is given in terms of four different folders: (1) VASP POSCARs for amorphous structures (called amorph_POSCARs), (2) VASP POSCARs for crystalline structures (called crystalline_nboxide_structures), (3) OCEAN outputs for amorphous structures (called amorph_U4), and (4) OCEAN outputs for crystalline structures (called cryst_U4). The &#39;amorph_U4&#39; folder contains subfolders for each structure, and within each subfolder is a &#39;Results&#39; folder containing the OCEAN input and output files, including individual XAS spectra for each individual oxygen atom in the structure. The organization of the &#39;cryst_U4&#39; folder structure is the same as the &#39;amorph_U4&#39; folder.</p> <p>To calculate the XAS spectra within the OCEAN code, we first performed DFT (using Quantum Espresso) with an energy cut-off of 92 Ryd., and a simplified Hubbard U of 4 eV was applied to the Nb <em>d</em> orbitals. The `O-high&#39; and `Nb-sp&#39; pseudopotentials from PseudoDojo were used. For the BSE, the electron orbitals were down-sampled onto real space grids chosen to match 1 grid point per 1 a.u., the k-point meshes were chosen to exceed 1 grid point per 0.16 a.u.<sup>-1</sup>, and the number of conduction bands was set to 0.126 times the unit cell volume (in a.u.<sup>3</sup>).&nbsp;<br> For the screening, electron orbitals were calculated on k-point meshes exceeding 1 grid point per 0.56 a.u.<sup>-1</sup>, and the number of conduction bands was set to 0.437 times the unit cell volume (in a.u.<sup>3</sup>).<br> A Lorentzian core-hole broadening of 0.07 eV was included, and additional Gaussian broadening of 0.5 eV was applied.</p>

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