<p indent=0mm>Solar energy is a clean and renewable source of energy. Various solar photovoltaic (PV) cell technologies have been developed, out of which perovskite PV cell technology is growing rapidly. Using organometal halide perovskite as an optical absorption component, the power conversion efficiency (PCE) of heterojunction solar PV cells increased from 3.8% in 2009 to 25.5% recently. Nonetheless, the bottleneck for CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>-based solar cells entering into commercial market is their poor stabilities relating to environmental, thermal, and ultraviolet light influence. In contrast, transition metal oxide perovskites are thermodynamically and chemically stable enough for solar cells’ commercialization, with more advantages such as bandgap (<italic>E</italic><sub>g</sub>) adjustability from <sc>0 to 6 eV,</sc> processing being compatible with transparent conducting oxides, and ferroelectric bulk PV effect. Owing to a wide <italic>E</italic><sub>g</sub>, traditional ferroelectric perovskite oxides exhibit poor visible optical absorption, low electrical conductivity, and thus extremely low PCE. As an alternative to p-n junction PV effect, ferroelectric bulk PV effect provides a new separation mechanism for photo-excited carriers, which is closely related to spatial inversion symmetry breaking and its resulting spontaneous electric polarization. Different from p-n junction, the active space for photo-excited carrier separation spans the whole ferroelectric body, and thus an above-<italic>E</italic><sub>g</sub> open-circuit voltage is produced. By narrowing <italic>E</italic><sub>g</sub> while maintaining ferroelectricity of oxide perovskites, ferroelectric semiconductors become available to monolithically integrate the p-n junction and ferroelectric bulk PV effects, which could, in principle, go beyond the Shockley-Queisser theoretical PCE limit of conventional<italic> </italic>p-n junction solar cells. Bismuth ferrite (BiFeO<sub>3</sub>) has been experimentally demonstrated to exhibit ferroelectric PV effect. Meanwhile, it has a high ferroelectric Curie temperature (<italic>T</italic><sub>C</sub>) of 830°C and an intermediate <italic>E</italic><sub>g</sub> of <sc>~2.2 eV,</sc> providing a large chemical space for solid solution perovskite oxides to trade off both target properties of narrow <italic>E</italic><sub>g</sub> and <italic>T</italic><sub>C</sub>><sc>400 K.</sc> In this report, 0.50BiFeO<sub>3</sub>-0.25A<sub>1</sub>MnO<sub>3</sub>-0.25A<sub>2</sub>TiO<sub>3</sub> (A<sub>1</sub> = Ca, Sr, Ba, A<sub>2</sub> = Sr, Ba, Pb) and 0.49BiFeO<sub>3</sub>-0.26BaTiO<sub>3</sub>-0.25(Sr<sub>1−</sub><sub><italic>x</italic></sub>Ba<sub><italic>x</italic></sub>)(Co<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub> (<italic>x </italic>= 0 and 0.4) ferroelectric semiconductors with <italic>E</italic><sub>g</sub> of <sc>~0.9 eV</sc> were created by substituting Fe<sup>3+</sup> with Mn<sup>4+</sup> or Co<sup>2+</sup> in BiFeO<sub>3</sub>-based solid solution perovskites. Ceramic samples were prepared using a refined solid-state reaction electroceramic processing. X-ray diffraction measurements showed them crystallized in a single pseudo-cubic perovskite phase, while Raman scattering characterizations illustrated a breaking of spatial inversion symmetry at room temperature. Optical absorbance measurements found that these Mn<sup>4+</sup>- or Co<sup>2+</sup>-substituted BiFeO<sub>3</sub>-based solid solution perovskites have a direct bandgap in a range of <sc>0.75–1.0 eV.</sc> Compared with CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> perovskites, their optical absorption reaches near-infrared band of solar spectra. Temperature-dependent resistance measurements showed their resistivity on the magnitude of order of <sc>~10<sup>6</sup> Ω cm</sc> with thermal excitation energy (<italic>E</italic><sub>a</sub>) of <sc>~0.5 eV.</sc> Combined with observation of frequency-dependent dielectric properties, A-site vacancies were proposed responsible for electrical conduction and dielectric relaxation. Through data-mining causal relationships between <italic>E</italic><sub>g</sub> and the filling number of d electron of B-site cations, <italic>μ</italic>×<italic>r</italic><sub>A</sub>/<italic>r</italic><sub>B</sub> ensemble descriptor of oxide perovskites (<italic>μ</italic>, <italic>r</italic><sub>A</sub>, and <italic>r</italic><sub>B</sub> are the reduced mass of primitive cell, A-site cation radius, and B-site cation radius, respectively), a physical model was proposed to predictively design chemical compositions of ferroelectric semiconducting oxide perovskites with <italic>E</italic><sub>g</sub><sc>~0.9 eV</sc> for applications of solar PV cells. This essay provides an opportunity for developing novel solar PV cells to integrate monolithically p-n junction and ferroelectric bulk PV effects, with PCE beyond the Shockley-Queisser theoretical limit.
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