3 research outputs found

    Carbon-Based CsPbBr<sub>3</sub> Perovskite Solar Cells: All-Ambient Processes and High Thermal Stability

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    The device instability has been an important issue for hybrid organic–inorganic halide perovskite solar cells (PSCs). This work intends to address this issue by exploiting inorganic perovskite (CsPbBr<sub>3</sub>) as light absorber, accompanied by replacing organic hole transport materials (HTM) and the metal electrode with a carbon electrode. All the fabrication processes (including those for CsPbBr<sub>3</sub> and the carbon electrode) in the PSCs are conducted in ambient atmosphere. Through a systematical optimization on the fabrication processes of CsPbBr<sub>3</sub> film, carbon-based PSCs (C-PSCs) obtained the highest power conversion efficiency (PCE) of about 5.0%, a relatively high value for inorganic perovskite-based PSCs. More importantly, after storage for 250 h at 80 °C, only 11.7% loss in PCE is observed for CsPbBr<sub>3</sub> C-PSCs, significantly lower than that for popular CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> C-PSCs (59.0%) and other reported PSCs, which indicated a promising thermal stability of CsPbBr<sub>3</sub> C-PSCs

    Highly Air-Stable Carbon-Based α‑CsPbI<sub>3</sub> Perovskite Solar Cells with a Broadened Optical Spectrum

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    Inorganic cesium lead halide perovskites with superb thermal stability show promise to fabricate long-term operational photovoltaic devices. However, the cubic phase (α) of CsPbI<sub>3</sub> with an appropriate band gap is unstable in air. We discover that highly stable α-CsPbI<sub>3</sub> can be obtained in dry air (temperature: 20–30 °C; humidity: 10–20%) by replacing PbI<sub>2</sub> with HPbI<sub>3</sub> in a one-step deposition solution. Furthermore, the band gap of HPbI<sub>3</sub>-processed α-CsPbI<sub>3</sub> is advantageously reduced from 1.72 to 1.68 eV due to the existence of tensile lattice strain. By employing such an α-CsPbI<sub>3</sub> film in carbon-based perovskite solar cells (C-PSCs), a power conversion efficiency (PCE) of 9.5% is achieved, which is a record value for the α-CsPbI<sub>3</sub> PSCs without hole transport material. Most importantly, over 90% of the initial PCE is retained for nonencapsulated devices after 3000 h of storage in dry air. Therefore, HPbI<sub>3</sub>-based one-step deposition presents a promising strategy to prepare high-performance and air-stable α-CsPbI<sub>3</sub> PSCs

    Colloidal Precursor-Induced Growth of Ultra-Even CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> for High-Performance Paintable Carbon-Based Perovskite Solar Cells

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    Carbon-based hole transport material (HTM)-free perovskite solar cells (PSCs) have attracted intense attention due to their relatively high stability. However, their power conversion efficiency (PCE) is still low, especially for the simplest paintable carbon-based PSCs (C-PSCs), whose performance is greatly limited by poor contact at the perovskite/carbon interface. To enhance interface contact, it is important to fabricate an even-surface perovskite layer in a porous scaffold, which is not usually feasible due to roughness of the crystal precursor. Herein, colloidal engineering is applied to replace the traditional crystal precursor with a colloidal precursor, in which a small amount of dimethyl sulfoxide (DMSO) is added into the conventional PbI<sub>2</sub> dimethylformamide (DMF) solution. After deposition, PbI<sub>2</sub>(DMSO) adduct colloids (which are approximately tens of nanometers in size) are stabilized and dispersed in DMF to form a colloidal film. Compared with PbI<sub>2</sub> and PbI<sub>2</sub>(DMSO) adduct crystal precursors deposited from pure DMF and DMSO solvents, respectively, the PbI<sub>2</sub>(DMSO) adduct colloidal precursor is highly mobile and flexible, allowing an ultra-even surface to be obtained in a TiO<sub>2</sub> porous scaffold. Furthermore, this ultra-even surface is well-maintained after chemical conversion to CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> in a CH<sub>3</sub>NH<sub>3</sub>I solution. As a result, the contact at the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>/carbon interface is significantly enhanced, which largely boosts the fill factor and PCE of C-PSCs. Impressively, the achieved champion PCE of 14.58% is among the highest reported for C-PSCs
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