Single‐Atom Ti Decorated Carbon Black and Carbon Nanotubes: Modular Dual‐Carbon Electrode for Optimizing the Charge Transport Kinetics of Perovskite Solar Cells

材料科学 碳纤维 电极 碳纳米管 动力学 电荷(物理) 钙钛矿(结构) 钙钛矿太阳能电池 对偶(语法数字) 化学物理 纳米技术 光电子学 化学工程 太阳能电池 复合材料 物理化学 复合数 艺术 工程类 文学类 化学 物理 量子力学
作者
Jiashuo Cheng,Hongru Ma,Yanying Shi,Lida Liu,Wenzhe Shang,Wei Liu,Si‐Ao Li,Wenrui Li,Yudi Wang,Yantao Shi
出处
期刊:Advanced Functional Materials [Wiley]
标识
DOI:10.1002/adfm.202409533
摘要

Abstract In the landscape of photovoltaic research, carbon‐based perovskite solar cells (C‐PSCs) have attracted widespread attention due to their outstanding stability. However, compared to metal‐based PSCs, their power conversion efficiency (PCE) lags markedly behind. The key lies in two primary factors: First, the inefficiency of the carbon electrode in transporting and collecting carriers; second, the energy level mismatch with adjacent functional layers. These problems increase both the charge transport resistance and the charge injection barriers, thereby diminishing the overall efficiency of the device. In this study, an effective strategy is presented to tackle this issue by developing modular C‐PSCs that utilize dual carbon electrodes and implement multiscale modulation. This approach specifically focuses on three crucial aspects: establishing a highly conductive network, ensuring sufficient interfacial contact, and achieving well‐matched energy band alignment. By synergistically incorporating 0D carbon black (CB) and 1D carbon nanotube (CNT) into dual carbon electrodes, a resilient conductive network with enhanced interfacial contact is established, creating favorable conditions for efficient carrier transfer. Additionally, the energy level structure of CB is meticulously adjusted at the molecular scale by introducing individually adsorbed titanium (Ti) atoms, effectively addressing the energy level mismatch with the hole transport layer (spiro‐OMeTAD), and notably reducing the charge injection barrier at the interface. Based on the above strategy, the PCE of the C‐PSCs has undergone a remarkable enhancement from 15.27% to 22.45%. Moreover, the device shows excellent stability, with its PCE retaining over 95% of the initial value even after 1000 h of continuous operation under one‐sun intensity.
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