Scalable Interfacial CsPbCl3 Layers as a Strain-Relief Strategy for Stable Perovskite/Silicon Tandem Cells
Oussama Er-raji a, Stephen Selvaraj a, Stefan W. Glunz a, Juliane Borchert a
a University of Freiburg, Department of Sustainable Systems Engineering (INATECH), Freiburg, 79110, Germany
b Fraunhofer Institute for Solar Energy Systems ISE, Germany, Heidenhofstraße, 2, Freiburg im Breisgau, Germany
Proceedings of MATSUS Fall 2026 Conference (MATSUSFall26)
A2 Multijunction Halide Perovskite Solar Cells: Materials, Device Design, and Advanced Characterization
Palma, Spain, 2026 October 26th - 30th
Organizers: Philip Schulz and Stefan Weber
Oral, Oussama Er-raji, presentation 326
Publication date: 22nd July 2026

As perovskite/silicon tandem solar cells approach their practical efficiency limit (35.2% experimentally vs. a 39.5% practical potential),[1,2] research focus is increasingly shifting toward scalable manufacturing and operational stability. Residual tensile strain in the perovskite layer remains an intrinsic challenge, arising from the mismatch in thermal expansion coefficients between the perovskite absorber and the silicon substrate.[3] This strain lowers the defect formation energy of halide vacancies, thereby accelerating device degradation.[4] Buried‑layer engineering, specifically introducing a thin 3D inorganic perovskite layer with a smaller lattice parameter than the photoactive perovskite, has recently been shown to counteract this tensile strain by imposing an external compressive strain.[5] Yet, the underlying deposition processes remain challenging to reproduce: cumbersome pure single crystal synthesis, in-situ annealing during thermal evaporation, and need for high post-annealing temperatures (200°C); thus limiting the broader technology transfer.

In this work, we develop a post-treatment-free thermal co‑evaporation process to deposit a 10 nm CsPbCl3 inorganic 3D perovskite layer beneath a 1.68 eV FA0.85Cs0.15Pb(I0.78Br0.22)3 photoactive absorber. The study systematically (1) maps the processing window required to obtain phase pure CsPbCl3 by tuning the CsCl/PbCl2 co evaporation rate ratio, assessed using XRD and steady-state PL; (2) investigates chlorine diffusion into the FA0.85Cs0.15Pb(I0.78Br0.22)3 absorber as a function of the CsPbCl3 post annealing temperature using ToF-SIMS; and (3) analyzes the charge extraction mechanism at the FACs/CsPbCl3/hole-transport-layer interface by optimizing the buried‑layer thickness and applying a combination of UPS, KPFM, transient PL, and device-level characterization (Suns-VOC and Suns-PL). In situ Bragg-Brentano XRD provides mechanistic insight into how the engineered inorganic layer modifies the crystallization pathway of the photoactive perovskite. Complementary grazing incidence XRD reveals the changes in residual strain within the target device stack. The derived design rules enable a scalable fabrication approach compatible with front side-textured silicon wafers featuring industry‑standard pyramid heights (> 2 µm), typically used in fully-textured perovskite/silicon tandem solar cells,[6] and presents a promising step towards stable and scalable next generation photovoltaics.

This work was funded by the German Federal Ministry for Economic Affairs and Climate Action under contract nos. 03EE1086A (PrEsto), 03EE1182A, and 03EE1182B (Perle). J.B. acknowledges support The Vector Stiftung for funding her research group.

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