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Published on: February 27, 2017
Buried Interface Engineering in Perovskite Solar Cells: Selective vs Spontaneous Heterointerface Modulation Using
Daisuke Kubota1,2, Atsushi Kogo1, Hiroyuki Yaguchi2
1National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Higashi, Tsukuba, Ibaraki 305-8565, Japan.
None:
Heterointerface modulation plays a crucial role in obtaining efficient perovskite solar cells (PSCs) owing to their multilayered architecture, which forms defect-prone heterointerfaces. Recently, spontaneous heterointerface modulation (SPHM) materials have emerged as additives for PSC component solutions and spontaneously modulate heterointerface(s) during solution deposition. Thus, SPHMs are advantageous because they eliminate the additional processes that conventional heterointerface modulators require and avoid atmospheric exposure of the modulated interface. Specifically, tetrafluoroborate (BF4-)-based materials exhibit SPHM functionalities; the BF4- anions spontaneously modulate the buried perovskite/electron transport material (ETM) interface in n-i-p PSC architectures. In principle, BF4-based additives are well suited to a narrow-bandgap FAPbI3 photoabsorber because the BF4- additives retain its narrow bandgap and can enhance photovoltaic performance. However, a limitation of FAPbI3 in the BF4-based SPHM system was recently identified: the BF4-composite deteriorates FAPbI3 bulk properties via its decomposition during the relatively high-temperature heating required for FAPbI3. As such issues may not be confined to BF4-based materials, the development of strategies for buried interface modulation using materials prone to decomposition is imperative. In this study, an ex situ treatment for the TiO2 surface is defined as selective heterointerface modulation (SEHM) and demonstrated its effectiveness for FAPbI3/ETM interface using a BF4-based material. SEHM with the BF4-based material negligibly affected the FAPbI3 bulk, unlike SPHM, yet effectively modulated the buried perovskite/ETM interface, demonstrating the unique benefit of SEHM relative to SPHM. Therefore, SEHM enhances photovoltaic performance via increasing open-circuit voltage, an improvement that SPHM did not achieve. Thus, SEHM proves to be a potent technology when employing such heterointerface modulators that are susceptible to decomposition, and it is generally applicable to materials beyond BF4-based systems. This work highlights the advantages and disadvantages of both SEHM and SPHM techniques and provides insights for the further development of nascent and potent SPHM, contributing to advancements in materials science.
