Abstract

Ferroelectric oxide perovskites are promising materials for use in photovoltaic devices, due to their ability to exploit the bulk photovoltaic effect to achieve high power-conversion efficiency. In this work, we use first-principles methods to investigate the ferroelectric perovskite $[{\mathrm{Ba}\mathrm{Ti}\mathrm{O}}_{3}{]}_{x}\text{\ensuremath{-}}[{\mathrm{Na}\mathrm{Ti}}_{1/2}{\mathrm{Mo}}_{1/2}{\mathrm{O}}_{3}{]}_{1\ensuremath{-}x}$ and $[{\mathrm{Ba}\mathrm{Ti}\mathrm{O}}_{3}{]}_{x}\text{\ensuremath{-}}[{\mathrm{Na}\mathrm{Ti}}_{1/2}{\mathrm{W}}_{1/2}{\mathrm{O}}_{3}{]}_{1\ensuremath{-}x}$ solid solutions for potential use in ferroelectric-based photovoltaics. We find that compositional variations change the band gap, shifting it to the edge of the visible range for the 25% ${\mathrm{Na}\mathrm{Ti}}_{1/2}{\mathrm{Mo}}_{1/2}{\mathrm{O}}_{3}$ composition and to the visible range for some Mo-cation and W-cation arrangements for the 50% ${\mathrm{Na}\mathrm{Ti}}_{1/2}{\mathrm{Mo}}_{1/2}{\mathrm{O}}_{3}$ and 50% ${\mathrm{Na}\mathrm{Ti}}_{1/2}{\mathrm{W}}_{1/2}{\mathrm{O}}_{3}$ compositions. Mo and W substitutions both maintain the ferroelectric properties of the parent ${\mathrm{Ba}\mathrm{Ti}\mathrm{O}}_{3}$. While the A-site cation arrangement has a minor effect on the band gap, the variations in the B-site cation arrangement and the cation displacements affect the band gap by up to 0.8 eV. Analysis of the structures and the calculated band-gap values shows that the band gap is controlled by the identity of the substituent cation, the O-B-O angles, the relative orientations of the Mo and W substituent atoms, and the B-cation displacement. We demonstrate the thermodynamic feasibility of these solid solutions by formation energy analysis. The decrease of the band gap relative to the parent ${\mathrm{Ba}\mathrm{Ti}\mathrm{O}}_{3}$ to the standard and transparent photovoltaic range combined with the ferroelectricity maintained make this earth-abundant-containing solid solution a promising candidate for use in high-performance ferroelectric-based photovoltaic devices.

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