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Nature (2026)
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Conventional n–i–p architecture remains a robust platform for scalable perovskite photovoltaics1,2, yet its steady-state efficiency has stagnated at about 26% (ref. 3), lagging behind their p–i–n counterparts4. This performance gap arises from persistent non-radiative recombination at textured electron transport layer (ETL)/perovskite interfaces, yet the underlying physical origin remains unknown. Here we show that these losses originate from the synergistic combination of band misalignment and electron accumulation at the buried interface. To address this dual challenge, we develop a continuously graded n+/n-doped SnO2 ETL through a ligand-competitive binding strategy, which enables spatially defined doping that creates a built-in electric field. This graded architecture simultaneously minimizes band offset and accelerates electron extraction, thereby effectively suppressing the cross-interface recombination. The resulting n–i–p perovskite solar cells (PSCs) achieve a certified steady-state power conversion efficiency (PCE) of 27.17% (27.50% in reverse scan), the highest for n–i–p PSCs reported so far. The scalability of this strategy is further demonstrated by achieving a PCE of 25.79% for a 1 cm2 device and 23.33% for a perovskite module with a 16.02 cm2 aperture area. This work establishes a generalized example for energy-band engineering in metal-oxide transport layers, overcoming a fundamental efficiency bottleneck in conventional perovskite photovoltaics.
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All data are available in the main text or the supplementary materials. Other data that support the findings of this study are available from the corresponding author upon request.
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We thank the staff of beamlines BL17B1, BL14B1, BL03HB, BL13SSW, BL13U and BL02U2 at SSRF for providing the beam time. This work was partly supported by Analysis Platform of New Matter Structure at Nankai University. This work was supported by the HE Research Fellowships from the HE Science Foundation.
This work is financially supported by the National Science Fund for Distinguished Young Scholars (grant no. T2225024), the Fundamental and Interdisciplinary Disciplines Breakthrough Plan of the Ministry of Education of China (JYB2025XDXM410), the Foundation for Innovative Research Groups of the National Natural Science Foundation of China (grant no. 22121005), the National Science Foundation (grant nos. 62261160389, 22475107, 224B2906, 22509015 and 525B2187) and the China National Postdoctoral Program for Innovative Talents (BX20250103). We extend our appreciation to the Deputyship for Research and Innovation, Ministry of Education in Saudi Arabia, for funding this research work (project no. IFKSU-DSR-NS-2026-1).
These authors contributed equally: Di Wang, Saisai Li, Zijin Ding
State Key Laboratory of Advanced Chemical Power Sources, Frontiers Science Center for New Organic Matter, Key Laboratory of Advanced Energy Materials Chemistry (Ministry of Education), Academy for Advanced Interdisciplinary Studies, College of Chemistry, Nankai University, Tianjin, People’s Republic of China
Di Wang (王迪), Saisai Li (李赛赛), Zijin Ding (丁紫津), Xingyu Chen (陈星宇), Qiao Zheng (郑樵), Keyu Wei (韦科妤), Yuanzhi Jiang (姜源植), Jun Chen (陈军) & Mingjian Yuan (袁明鉴)
School of Interdisciplinary Science, Beijing Institute of Technology, Beijing, People’s Republic of China
Jian Xu (徐健)
Department of Physics, College of Science, Princess Nourah Bint Abdulrahman University, Riyadh, Saudi Arabia
Thamraa Alshahrani
Nano-Science Center and Department of Chemistry, University of Copenhagen, Copenhagen, Denmark
Siyu Liu (刘思宇)
College of Physics Science and Technology, Hebei University, Baoding, People’s Republic of China
Tingwei He (何庭伟)
Ultrafast Electron Microscopy Laboratory, The MOE Key Laboratory of Weak-Light Nonlinear Photonics, College of Physics, Nankai University, Tianjin, People’s Republic of China
Xinxin Yue (岳鑫欣) & Xuewen Fu (付学文)
Department of Physics and Astronomy, College of Science, King Saud University, Riyadh, Saudi Arabia
Saif M. H. Qaid
PHI Analytical Laboratory, ULVAC-PHI Instruments, Nanjing, People’s Republic of China
Lin Feng (冯林), Ou Yang (杨欧) & Huanxin Ju (鞠焕鑫)
Haihe Laboratory of Sustainable Chemical Transformations, Tianjin, People’s Republic of China
Yuanzhi Jiang (姜源植), Jun Chen (陈军) & Mingjian Yuan (袁明鉴)
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M.Y. conceived the idea. M.Y. and J.C. supervised the project. D.W. and Z.D. fabricated the devices. J.X. did the DFT and AIMD calculations. X.C. did the 31P-NMR test. S. Liu., K.W., X.F., Y.J. and X.Y. did the TR measurement and analysis. H.J., L.F., O.Y., T.H., D.W. and S. Li were responsible for IPES, HAXPES and TOF-SIMS characterization. D.W., Q.Z., T.H., T.A., S.M.H.Q. and S. Li carried out the electrical and optical characterization. M.Y. and D.W. co-wrote the paper. All the authors contributed to the discussion and commented on the paper.
Correspondence to Jian Xu (徐健), Yuanzhi Jiang (姜源植) or Mingjian Yuan (袁明鉴).
The authors have filed a provisional patent for this work to the China National Intellectual Property Administration (CNIPA).
Nature thanks Thad Druffel, Deying Luo and the other, anonymous, reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
The certified steady-state PCEs (>25%) and the corresponding Voc loss reported to date for PSCs in both n–i–p and p-i-n configurations44,45,46,47,48,49,50,51,52,53,54.
J–V curves for n–i–p devices based on control-SnO2 ETL (a) and continuously graded-doped SnO2 ETL (b). J–V curves of PSCs based on continuously graded-doped SnO2 ETL for a 1 cm2 device (c) and a 5 × 5 cm2 solar module (d), respectively.
a, Cross-sectional HAADF-STEM images of conformal SnO2 ETLs with varying thicknesses as a function of deposition time. b, TEM image of SnO2 NPs (3–5 nm) in solution (i), and cross-sectional TEM images of the corresponding SnO2 film, showing a uniform assembly of nanoparticles with diameters of 3–5 nm (ii, iii).
a, Schematic diagram of electrostatic assembly of SnO2 NPs capped with bidentate ligands. b, Molecular structures of the introduced bidentate ligands (left) and their corresponding configurations under acidic conditions (pH = 1.5–3) (right). SEM images (c), zeta potential (d) and CV measurements (e) for SnO2 capped with ET, TA, TGA, TE ligands.
Supplementary Notes 1–12, including Supplementary Figs. 1–54, Supplementary Tables 1–7 and additional references.
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Wang, D., Li, S., Ding, Z. et al. Continuously graded-doped SnO2 for efficient n–i–p perovskite solar cells. Nature (2026). https://doi.org/10.1038/s41586-026-10587-4
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