• Journal of Semiconductors
  • Vol. 43, Issue 3, 030501 (2022)
Tian Tian1, Meifang Yang1, Jianyu Yang1, Wuqiang Wu1, and Liming Ding2
Author Affiliations
  • 1Key Laboratory of Bioinorganic and Synthetic Chemistry (MoE), Lehn Institute of Functional Materials, School of Chemistry, Sun Yat-sen University, Guangzhou 510006, China
  • 2Center for Excellence in Nanoscience (CAS), Key Laboratory of Nanosystem and Hierarchical Fabrication (CAS), National Center for Nanoscience and Technology, Beijing 100190, China
  • show less
    DOI: 10.1088/1674-4926/43/3/030501 Cite this Article
    Tian Tian, Meifang Yang, Jianyu Yang, Wuqiang Wu, Liming Ding. Stabilizing black-phase CsPbI3 under over 70% humidity[J]. Journal of Semiconductors, 2022, 43(3): 030501 Copy Citation Text show less

    Abstract

    Abstract

    Recently, all-inorganic perovskites have attracted attention due to good thermal stability[1-12]. Among them, CsPbI3 has the most desirable optical bandgap (~1.7 eV) for applications in optoelectronic devices[13-16]. In general, making black-phase CsPbI3 film requires a high-temperature annealing up to 320 °C[17, 18], which inevitably raises energy consumption. Though being made at high temperature, the resulting black-phase (α or β phase) CsPbI3 film still suffers from an undesirable phase transition under ambient conditions[19, 20]. Several strategies have been developed to lower the annealing temperature (90–100 °C)[20-26], it is still challenging to stabilize black-phase CsPbI3 under ambient condition with high humidity and without a tedious annealing process. Herein, we developed a simple crystal redissolution (CR) strategy to make stable black-phase CsPbI3 film in ambient air with high humidity and without post-annealing. 4-N,N-dimethylamino-4ʹ-Nʹ-methyl-stilbazolium tosylate (DAST) can chemically interact with CsPbI3 to reduce the formation energy of black-phase and inhibit CsPbI3 to undergo black-to-yellow phase transition.

    Fig. 1(a) shows the CR approach. By using the perovskite precursor consisting of PbI2, CsI and HI, a light-yellow film was obtained in ambient air, which is due to the existence of both yellow-phase δ-CsPbI3 and PbI2, as evidenced in XRD pattern (Fig. 1(b))[22]. In contrast, by using CR-derived perovskite precursor (Fig. S1), a mirror-like black CsPbI3 film was obtained even under 70% relative humidity, which uniformly covered the entire substrate (inset in Fig. 1(c)). Compared with the control sample (Fig. 1(b)), there is no PbI2 signal (12.6°) in XRD pattern (Fig. 1(c))[27], which is due to a more direct conversion and rapid self-assembly from CsPbI3 crystals to CsPbI3 film, rather than the complicated competition among Pb2+, Cs+, I ions and solvent molecules[27, 28]. The diffraction peaks at 14.98° and 29.20° are the typical (100) and (200) planes of black-phase β-CsPbI3. Meanwhile, the absorbance of the control film sharply declined after 450 nm, while CR-derived black CsPbI3 film presents an absorption onset at 733 nm (Fig. S2), which agrees with the previous report on β-CsPbI3 film[12]. For the control film, inferior surface coverage was observed (Figs. S3(a) and S3(c)). And CR-derived film shows better surface coverage (Figs. S3(b) and S3(d)).

    (Color online) (a) The ambient air-processed black-phase CsPbI3 film via CR strategy. The XRD patterns of the control (b) and CR-derived CsPbI3 film (c). Note: the hash key represents the signal from δ-CsPbI3; the square symbol represents the signal from PbI2; the diamond symbol represents the signal from β-CsPbI3; the circular pattern represents the signal from CsI and the asterisk represents the signal from FTO glass substrate. (d) The structure of DAST. (e) Schematic for the molecular interaction and CsPbI3 film formation. (f) The XRD pattern for DAST-modified CsPbI3 film after being stored in air for one month.

    Figure 1.(Color online) (a) The ambient air-processed black-phase CsPbI3 film via CR strategy. The XRD patterns of the control (b) and CR-derived CsPbI3 film (c). Note: the hash key represents the signal from δ-CsPbI3; the square symbol represents the signal from PbI2; the diamond symbol represents the signal from β-CsPbI3; the circular pattern represents the signal from CsI and the asterisk represents the signal from FTO glass substrate. (d) The structure of DAST. (e) Schematic for the molecular interaction and CsPbI3 film formation. (f) The XRD pattern for DAST-modified CsPbI3 film after being stored in air for one month.

    Black-phase CsPbI3 film gradually degraded and underwent phase transition when stored in air for one week, as evidenced by the gradual decrease of absorbance (Fig. S4). To further improve phase stability and optoelectronic properties of β-CsPbI3 film prepared by CR strategy, we introduced the DAST additive (Fig. 1(d)). DAST not only maintains black-phase CsPbI3 structure, but also slightly enhances the crystallinity and promotes the crystal growth orientation along (100) and (200) planes (Fig. S5). DAST also helps to reduce the grain sizes (100–200 nm) and improve the surface coverage of the resultant β-CsPbI3 film (Fig. S6). DAST molecules can interact with CsPbI3via robust bidentate coordination, thus impeding grain growth due to the steric hindrance effect (Fig. 1(e))[11]. The interaction between DAST molecule and β-CsPbI3 was studied by FTIR (Fig. S7). The pure DAST shows characteristic signals at 1023 and 1666 cm–1, corresponding to C=C bond and benzene group, respectively. DAST-modified CsPbI3 film also shows similar peaks, but with a slight shift, suggesting possible interaction between zwitterion and ions in perovskites[20]. The DAST-modified CsPbI3 film was stored at room temperature in air with a relative humidity of ~35%. There was no obvious degradation observed even after one month, as proved by XRD pattern (Fig. 1(f)).

    In short, by using the CR strategy, we successfully stabilized the black-phase CsPbI₃ film in ambient air with >70% humidity. DAST can further stabilize the black phase. The approaches in this work will be useful for developing efficient perovskite solar cells.

    Acknowledgements

    We appreciate the National Natural Science Foundation of China (22005355) and Guangdong Basic and Applied Basic Research Foundation (2019A1515110770). L. Ding thanks the National Key Research and Development Program of China (2017YFA0206600) and the National Natural Science Foundation of China (51773045, 21772030, 51922032, 21961160720) for financial support.

    Appendix A. Supplementary materials

    References

    [1] R J Sutton, G E Eperon, L Miranda et al. Bandgap-tunable cesium lead halide perovskites with high thermal stability for efficient solar cells. Adv Energy Mater, 6, 1502458(2016).

    [2] L Lin, L Jiang, P Li et al. Simulated development and optimized performance of CsPbI3 based all-inorganic perovskite solar cells. Solar Energy, 198, 454(2020).

    [3] B Yu, C Zuo, J Shi et al. Defect engineering on all-inorganic perovskite solar cells for high efficiency. J Semicond, 42, 050203(2021).

    [4] Y Tang, A Lesage, P Schall. CsPbI3 nanocrystal films: towards higher stability and efficiency. J Mater Chem C, 8, 17139(2020).

    [5] A Swarnkar, A R Marshall, E M Sanehira et al. Quantum dot-induced phase stabilization of α-CsPbI3 perovskite for high-efficiency photovoltaics. Science, 354, 92(2016).

    [6] R J Sutton, M R Filip, A A Haghighirad et al. Cubic or orthorhombic? Revealing the crystal structure of metastable black-phase CsPbI3 by theory and experiment.. ACS Energy Lett, 3, 1787(2018).

    [7] D B Straus, S Guo, A M Abeykoon et al. Understanding the instability of the halide perovskite CsPbI3 through temperature-dependent structural analysis. Adv Mater, 32, 2001069(2020).

    [8] B Li, Y Zhang, L Fu et al. Surface passivation engineering strategy to fully-inorganic cubic CsPbI3 perovskites for high-performance solar cells. Nat Commun, 9, 1076(2018).

    [9] F Ke, C Wang, C Jia et al. Preserving a robust CsPbI3 perovskite phase via pressure-directed octahedral tilt. Nat Commun, 12, 461(2021).

    [10] Q Huang, F Li, M Wang et al. Vapor-deposited CsPbI3 solar cells demonstrate an efficiency of 16%. Sci Bull, 66, 757(2021).

    [11] Q Wang, X Zheng, Y Deng et al. Stabilizing the α-Phase of CsPbI3 perovskite by sulfobetaine zwitterions in one-step spin-coating films. Joule, 1, 371(2017).

    [12] K Wang, Z Jin, L Liang et al. All-inorganic cesium lead iodide perovskite solar cells with stabilized efficiency beyond 15%. Nat Commun, 9, 4544(2018).

    [13] T Zhang, F Wang, H Chen et al. Mediator-antisolvent strategy to stabilize all-inorganic CsPbI3 for perovskite solar cells with efficiency exceeding 16%. ACS Energy Lett, 5, 1619(2020).

    [14] Y Hu, F Bai, X Liu et al. Bismuth incorporation stabilized α-CsPbI3 for fully inorganic perovskite solar cells. ACS Energy Lett, 2, 2219(2017).

    [15] D P McMeekin, G Sadoughi, W Rehman et al. A mixed-cation lead mixed-halide perovskite absorber for tandem solar cells. Science, 351, 151(2016).

    [16] R E Beal, D J Slotcavage, T Leijtens et al. Cesium lead halide perovskites with improved stability for tandem solar cells. J Phys Chem Lett, 7, 746(2016).

    [17] G E Eperon, G M Paternò, R J Sutton et al. Inorganic caesium lead iodide perovskite solar cells. J Mater Chem A, 3, 19688(2015).

    [18] E M Hutter, R J Sutton, S Chandrashekar et al. Vapour-deposited cesium lead iodide perovskites: microsecond charge carrier lifetimes and enhanced photovoltaic performance. ACS Energy Lett, 2, 1901(2017).

    [19] Y Wang, T Zhang, M Kan et al. Efficient α-CsPbI3 photovoltaics with surface terminated organic cations. Joule, 2, 2065(2018).

    [20] X Xu, H Zhang, E Li et al. Electron-enriched thione enables strong Pb-S interaction for stabilizing high quality CsPbI3 perovskite films with low-temperature processing. Chem Sci, 11, 3132(2020).

    [21] S M Yoon, H Min, J B Kim et al. Surface engineering of ambient-air-processed cesium lead triiodide layers for efficient solar cells. Joule, 5, 183(2021).

    [22] T Zhang, M I Dar, G Li et al. Bication lead iodide 2D perovskite component to stabilize inorganic α-CsPbI3 perovskite phase for high-efficiency solar cells. Sci Adv, 3, e1700841(2017).

    [23] J Zhang, J Liu, A Tan et al. Improved stability of β-CsPbI3 inorganic perovskite using π-conjugated bifunctional surface capped organic cations for high performance photovoltaics. Chem Commun, 56, 13816(2020).

    [24] T Ye, L Pan, Y Yang et al. Synthesis of highly-oriented black CsPbI3 microstructures for high-performance solar cells. Chem Mater, 32, 3235(2020).

    [25] Y Wang, J Yuan, X Zhang et al. Surface ligand management aided by a secondary amine enables increased synthesis yield of CsPbI3 perovskite quantum dots and high photovoltaic performance. Adv Mater, 32, 2000449(2020).

    [26] C Wang, A S R Chesman, J J Jasieniak. Stabilizing the cubic perovskite phase of CsPbI3 nanocrystals by using an alkyl phosphinic acid. Chem Commun, 53, 232(2017).

    [27] J Shi, Y Wang, Y Zhao. Inorganic CsPbI3 perovskites toward high-efficiency photovoltaics. Energy Environ Mater, 2, 73(2019).

    [28] Z Zhang, J Li, Z Fang et al. Adjusting energy level alignment between HTL and CsPbI2Br to improve solar cell efficiency. J Semicond, 42, 030501(2021).

    Tian Tian, Meifang Yang, Jianyu Yang, Wuqiang Wu, Liming Ding. Stabilizing black-phase CsPbI3 under over 70% humidity[J]. Journal of Semiconductors, 2022, 43(3): 030501
    Download Citation