Robust perovskite formation via vacuum thermal annealing for indoor perovskite solar cells

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作者
Kwanchai Penpong
Chaowaphat Seriwatanachai
Atittaya Naikaew
Napan Phuphathanaphong
Ko Ko Shin Thant
Ladda Srathongsian
Thunrada Sukwiboon
Anuchytt Inna
Somboon Sahasithiwat
Pasit Pakawatpanurut
Duangmanee Wongratanaphisan
Pipat Ruankham
Pongsakorn Kanjanaboos
机构
[1] Mahidol University,School of Materials Science and Innovation, Faculty of Science
[2] Ministry of Higher Education,Center of Excellence for Innovation in Chemistry (PERCH
[3] Science,CIC)
[4] Research and Innovation,Department of Chemistry, Faculty of Science
[5] National Metal and Materials Technology Center (MTEC),Department of Physics and Materials Science, Faculty of Science
[6] Mahidol University,undefined
[7] Chiang Mai University,undefined
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Scientific Reports | / 13卷
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摘要
Perovskite materials are fascinating candidates for the next-generation solar devices. With long charge carrier lifetime, metal-halide perovskites are known to be good candidates for low-light harvesting. To match the irradiance spectra of indoor light, we configured a triple-cation perovskite material with appropriate content of bromide and chloride (FA0.45MA0.49Cs0.06Pb(I0.62Br0.32Cl0.06)3) to achieve an optimum band gap (Eg) of ∼\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sim$$\end{document}1.80 eV. With low photon flux at indoor condition, minimal recombination is highly desirable. To achieve such goal, we, for the first time, combined dual usage of antisolvent deposition and vacuum thermal annealing, namely VTA, to fabricate a high-quality perovskite film. VTA leads to compact, dense, and hard morphology while suppressing trap states at surfaces and grain boundaries, which are key culprits for exciton losses. With low-cost carbon electrode architecture, VTA devices exhibited average power conversion efficiency (PCE) of 27.7 ± 2.7% with peak PCE of 32.0% (Shockley–Queisser limit of 50–60%) and average open-circuit voltage (Voc) of 0.93 ± 0.02 V with peak Voc of 0.96 V, significantly more than those of control and the vacuum treatment prior to heat.
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