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Article

Getting to the Heart of the Matter: Control over the Photolysis of PbI2 Through Partial Lead Substitution

by
Marina I. Ustinova
1,2,
Gennadii V. Shilov
1,
Pavel A. Troshin
1,3,*,
Sergey M. Aldoshin
1 and
Lyubov A. Frolova
1,*
1
Federal Research Center for Problems of Chemical Physics and Medicinal Chemistry of the Russian Academy of Sciences, 1 prosp. Semenova, 142432 Chernogolovka, Russia
2
CHOSE (Centre for Hybrid and Organic Solar Energy), Department of Electronic Engineering, University of Rome Tor Vergata, Casale 11, 00133 Rome, Italy
3
Zhengzhou Research Institute of HIT, Longyuan East 7th 26, Jinshui District, Zhengzhou 450003, China
*
Authors to whom correspondence should be addressed.
Inorganics 2025, 13(1), 13; https://doi.org/10.3390/inorganics13010013
Submission received: 26 November 2024 / Revised: 25 December 2024 / Accepted: 3 January 2025 / Published: 6 January 2025
(This article belongs to the Special Issue New Semiconductor Materials for Energy Conversion)

Abstract

A crucial problem of the photoinduced degradation of perovskite semiconductors based on complex lead halides has been addressed here by suppressing PbI2 photolysis to metallic lead. The systematic screening of >30 modifying cations introduced as substituents for 5% of Pb2+ in the PbI2 composition has revealed their tremendous effects on the rate of material degradation under light exposure. Thus, the most successful stabilizing cations could maintain a high absorbance of the Pb0.95M0.1/nI2 films and block Pb0 formation after 400 h of continuous illumination, when the non-modified PbI2 films completely decomposed to Pb0 and I2. The obtained results present a promising solution for the problem of metallic lead formation in the active layer of perovskite solar cells during their operation, which can pave the way for the development of a new generation of highly efficient and stable perovskite photovoltaics.

1. Introduction

Complex lead halides with the perovskite crystal structure APbX3, where A is a univalent cation of methylammonium (MA), formamidinium (FA), or cesium, and X is the halide anion (I, Br, or Cl), have attracted tremendous attention from researchers and industry due to their excellent semiconductor properties combined with unprecedented defect tolerance. The perovskite solar cells (PSCs) based on these materials emerged rapidly within the last decade and demonstrated certified power conversion efficiencies exceeding 26% [1]. Furthermore, PSCs have the benefits of the relatively simple and cost-effective technology of their production and abundance of all raw materials, which are the major prerequisites of third-generation photovoltaic (PV) technology [2,3,4,5,6]. However, the low stability of complex lead halides with respect to light, elevated temperatures, and humidity hinders the commercialization of PSCs [7].
The photoinduced degradation of the absorber materials produced at the first stage of binary lead iodide PbI2 does not impair the photovoltaic performance of PSCs very much [8]. On the contrary, PbI2 is intentionally introduced into the perovskite absorber layer to improve the performance of PSCs, particularly those assembled using the n-i-p configuration [9]. This is believed to passivate defect states at the grain boundaries of the perovskite absorber material and thus suppresses the non-radiative recombination of charge carriers [10,11,12]. Furthermore, PbI2 could react back with the volatile organic products formed by photoinduced or thermal decomposition of complex lead halides and thus regenerate the perovskite absorber material [8]. This effect is largely responsible for the self-healing behavior of perovskite solar cells [13]. However, PbI2 itself undergoes facile photolysis and produces metallic lead Pb0 [8,14,15], which induces the massive recombination of charge carriers, leading to rapid decay in PSC performance [16]. Furthermore, another PbI2 photolysis product, the molecular iodine I2, is exceptionally corrosive, even in the form of the triiodide anion I3, and it aggressively reacts with the top electrode material, just forming an insulating metal iodide interlayer and leading finally to PSC device failure [17,18]. Thus, blocking the photolysis of PbI2 in the absorber layer of perovskite solar cells represents an urgent and crucially important task for achieving the required long-term stability of PSCs.
This challenge has been addressed recently by combining PbI2 with RbCl in n-i-p PSCs, which resulted in the formation of some complex that was more stable than pristine PbI2, so such a modification enhanced the operational stability of PSCs [19]. Alternatively, some organic additives were employed to improve the resistance of PbI2 to light, e.g., semicarbazide hydrochloride [20], 2-thiophenecarboxamide [21], or tryptophan [22]. However, similar reports are very scarce, and the performance of the proposed PbI2 stabilization approaches has not been verified directly in intrinsic photostability tests.
Herein, we present an alternative approach to control the photolysis of PbI2 through the partial substitution of Pb2+ cations in their composition by other rationally chosen metal ions. We have demonstrated previously that the photostability of all inorganic CsPbI3 and hybrid MAPbI3 could substantially be enhanced due to the introduction of certain substituent metal ions, which were found to be different for different material compositions [23,24]. We observed that in some cases, the formation of metallic lead was considerably or even completely suppressed, which inspired us to search for material compositions that would solve the problem of PbI2 photolysis.

2. Results and Discussion

Altogether, we screened >30 different substituent metal ions in thin films of Pb0.95M0.1/nI2 (where Mn+ is the substituent cation) compositions. It should be emphasized that the vast majority of the introduced modifying Mn+ cations could not occupy Pb2+ positions in the crystal lattice or can only be included in the perovskite lattice to a low extent due to the ion size mismatch and/or for other reasons; therefore, the corresponding MIn phase is localized mostly on the surface of PbI2 grains or at the grain boundaries. The localization of the introduced Mn+ cations has not been investigated thoroughly in this work since we were focused more on achieving the practically important result, i.e., enhancing the photostability of PbI2. However, interested readers can refer to our recent study of lead substitution in MAPbI3, where the substituent ion localization has been analyzed in detail [24]. In the case of the structural replacement of Pb2+ in the PbI2 lattice at low substitution levels (about 1%), when the cations have an oxidation state of 1+ (M+), the electroneutrality can be achieved by the local compensation of the negative charge by positively charged vacancies of I or by h+ capture, and in the case of M3+/4+, it is possible by interstitial I or e capture. At high substitution levels (>1%), when the oxidation state of the substituting cation is +3, the electroneutrality can be preserved by replacing Pb2+ with M3+ due to the formation of Pb2+ vacancies (VPb2−). In addition, there are previous works showing that layered crystalline systems (PbI2)1−x(MIn)x, where n = 1–3, often represent non-mixing alternating individual nanoclusters or layers enriched with lead iodide and metal iodide, which can impart their tunable semiconductor properties [25,26,27].
The intrinsic photostability of the Pb0.95M0.1/nI2 films was investigated in an inert atmosphere of pure nitrogen (O2 and H2O levels below 0.1 ppm) under exposure to the white light provided by an LED array with an incident intensity of 85 mW/cm2. However, considering the spectral irradiance of the light source and the absorption spectrum of PbI2, the number of the photons absorbed by the samples under the used test conditions corresponds to the value obtained under the ~150 mW/cm2 irradiation with the true AM1.5G solar spectrum. The equilibrium sample temperature was quite low (32 °C), so the heat did not play a major role in accelerating the PbI2 photolysis reaction [28].
The photoinduced aging of the Pb0.95M0.1/nI2 films was monitored by periodically measuring the UV-Vis optical spectra of the films (Figures S1–S8, Electronic Supplementary Materials (ESMs)). The films of pristine PbI2 undergo rapid photobleaching, as shown in Figure 1a. However, some of the material formulations demonstrated much superior resistance to light, as illustrated by the behavior of Pb0.95Fe0.05I2 in Figure 1b. A wavelength of 360 nm was used to analyze the time dynamics of the photolysis reaction by plotting the normalized absorbance as a function of the aging time t (see below). The values of the normalized absorbance of Pb0.95M0.1/nI2 films obtained after 400 h of aging (A400/A0) are presented in Figure 1c for each of the studied metal cations. Interestingly, all the studied substituents, except for Hg2+, improve the photostability of the PbI2 films. The highest photostability was revealed for the films modified with Bi3+, Eu2+/3+, Pt2+, Zn2+, Fe2+, Co2+, and Ag+ cations. The analysis of the phase composition of the aged Pb0.95M0.1/nI2 films using X-ray diffraction (XRD) revealed the absence of the crystalline phase of metallic lead (Pb0) in all the systems that were found to be the most stable according to the UV-Vis spectroscopy data (Figure 1d, Figures S9–S11, ESMs). It is worth mentioning that the stabilization effect of Ag+ introduced in the form of AgI is very surprising since silver iodide is known for its exceptionally high light sensitivity and is widely exploited in the film photography industry.
We have analyzed the dynamics of the photoinduced decomposition of Pb0.95M0.1/nI2 films and plotted the normalized absorbance of the films At/A0 as a function of the aging time, as shown in Figure S12 (ESMs), for all studied systems and in Figure 2a for a selected group of cations. One could notice that the thin films of the reference PbI2 and Pb0.95Hg0.05I2 degrade considerably more rapidly than other material formulations presented in Figure 2a. It has been found that their aging behavior is well described by the third-order reaction kinetics, as can be concluded from the linear dependence of (At/A0)−2 vs. aging time (Figure 2d).
Similar behavior among all the studied systems was found only for Pb0.95Y0.1/3I2, but this material shows much slower degradation dynamics manifested in a smaller slope of the fitted curve in Figure 2d and, hence, a lower rate constant as compared to that of PbI2 and Pb0.95Hg0.05I2. The formal third order of the photolysis reaction points to its complicated mechanism and suggests that the aging products catalyze the degradation of the starting material. Such an observation has been made previously for the photoinduced degradation of MAPbI3 films and was supported by several microscopy techniques [14]. The second-order reaction kinetics have been observed for the samples modified by Yb2+, In3+, and Lu3+ (Figure 2c). Multiple systems, including the most stable materials incorporating Eu2+/3+ and Bi3+ cations, have demonstrated first-order reaction kinetics (Figure 2b). For other studied systems, the aging kinetics cannot be fitted with any reasonable accuracy with such simple equations, so the reaction order represents some fractional number.
The obtained results demonstrated the tremendous effects of the modifying metal cations on the photolysis rate of the Pb0.95M0.1/nI2 films. This is clearly seen in the absorption dynamics shown in Figure 2a (and Figure S12) and also in the very different slopes of the kinetic curves presented, for example, in Figure 2b. Thus, the introduced substituent cations can block some of the elementary acts of PbI2 photolysis and thus decelerate this undesired process. Even though we cannot study the elementary acts of the PbI2 photolysis reaction with the available experimental techniques, we could speculate about some of the possible action mechanisms for the most efficient PbI2 stabilizers: Eu2+/3+ and Bi3+ cations. In the case of europium, it has the unique Eu2+/Eu3+ redox potential, matching that of Pb2+/Pb0 in the perovskite precursor solution, so mixing pure Eu2+ results in its partial oxidation to Eu3+ accompanied by the Pb2+ reduction to Pb0. However, all these processes are reversible, so Eu2+/Eu3+ acts as a redox shuttle, promoting the recombination of the photogenerated Pb0 and I2 (I3) and extending the lifetime of the perovskite films [29,30]. We believe that similar redox chemistry involving the Eu2+/Eu3+ pair is responsible for the observed stabilization of PbI2 under light exposure.
Another stabilizing cation, Bi3+, is known for its ability to trap molecular iodine and form polyiodides [31], which leads, as we believe, to the realization of a very similar stabilization pathway as Eu2+/Eu3+. Thus, the photolysis of non-modified PbI2 produces molecular iodine that evaporates from the aged film to the environment, thus making the reaction irreversible. On the contrary, in the modified films, the photogenerated I2 could efficiently be trapped either by Eu2+ (the redox reaction produces Eu3+ and I) or by BiI3 (the reaction produces polyiodide complexes), so the formed species stay in the film and have enough time to react back with Pb0, reforming Pb2+ and thus regenerating PbI2.

3. Materials and Methods

3.1. Materials

Borosilicate glass slides (25 × 25 mm) used as substrates were purchased from Isolab GmbH, (Eschau, Germany). Anhydrous dimethyl formamide (DMF) used as solvent was purchased from Sigma-Aldrich and used as received inside nitrogen glove boxes. The following anhydrous reagents and solvents were purchased from Sigma-Aldrich (St. Louis, MO, USA): PbI2, CaI2, SrI2, BaI2, PtI2, EuI2, SnI4, SnI2, MnI2, FeI2, CoI2, CuI, AgI, ZnI2, HgI2, CdI2, and SbI3 (purity 99.999%); YI3, NdI3, DyI2, YbI2, and LuI3 (purity 99.9%); GeI2 (purity 99.8%); MgI2, BiI3, and InI3 (purity 99.998%); and NiI2, LaI3, CeI3, ErI3, TbI3, and GdI3 (purity 99.99%).

3.2. Preparation of the PbI2 and Pb0.95M0.1/nI2 Films

3.2.1. Substrate Preparation

The glass substrates were cleaned sequentially with deionized water, acetone, and toluene followed by the RF air plasma treatment for 5 min. All further manipulations were performed inside nitrogen glove boxes under a well-controlled atmosphere.

3.2.2. Preparation of Precursor Solutions Based on Lead Iodide

The Pb0.95M0.1/nI2 precursor solutions with a concentration of 0.3 M were obtained by dissolving together 0.285 mmol of PbI2 and 0.3/n mmol of MIn in 1 mL of anhydrous DMF under continuous stirring at room temperature.

3.2.3. Deposition of the Films Based on Lead Iodide

The 45 µL aliquots of the corresponding precursor solutions were dropped on glass substrates rotating at 3000 rpm. The obtained films were annealed at 90 °C for 30 min in an inert atmosphere of the glove box to ensure the elimination of the solvent molecules and the proper crystallization of the modified PbI2 film.

3.3. Photostability Testing

The aging tests were carried out under continuous illumination using a special setup placed inside MBraun gloveboxes with an inert nitrogen atmosphere (O2 and H2O < 1 ppm). White light with a power of 85 ± 10 mW/cm2 was provided by LED arrays. The temperature of the samples was within the range of 32 ± 2 °C.

3.4. Pb0.95M0.1/nI2 Film Characterization

The UV-Vis absorption spectra were obtained using an AvaSpec-2048-2 UV-VIS fiber spectrometer integrated inside a glove box (Advantest corporation, Tokyo, Japan). The X-ray diffraction (XRD) patterns were collected using an Aeris instrument (Malvern PANalytical B.V., Malvern, UK) with the CuKα source.

4. Conclusions

To summarize, we have explored, for the first time, the potential of ion substitution chemistry as a simple but efficient approach to control the photoinduced decomposition of PbI2 films. The obtained results demonstrated a tremendous enhancement of PbI2 stability due to the introduction of optimum substituent ions such as Bi3+, Eu2+/3+, Pt2+, Zn2+, Fe2+, Co2+, and Ag+ cations. The modified films maintained high absorbance and showed no metallic lead formation detectable by XRD after 400 h of continuous illumination, while pristine non-modified PbI2 completely decomposed under these conditions. The obtained results are crucially important in the context of improving the photostability of the lead halide perovskite absorber materials and pave the way to the development of perovskite solar cells with long operational lifetimes.

Supplementary Materials

The following supporting information can be downloaded at https://www.mdpi.com/article/10.3390/inorganics13010013/s1, Figure S1: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Bi3+ (a), Eu2+ (b) Pt2+ (c), and Zn2+ (d) upon white light exposure, Figure S2: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Co2+ (a), Ag+ (b) Ca2+ (c), and Ce2+ (d) upon white light exposure, Figure S3: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Nd3+ (a), Sn2+ (b) Ni2+ (c), and La3+ (d) upon white light exposure, Figure S4: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Sb3+ (a), Sr2+ (b) Ba2+ (c), and Mn3+ (d) upon white light exposure, Figure S5: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Tb3+ (a), Y3+ (b) Cd2+ (c), and Dy2+ (d) upon white light exposure, Figure S6: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = In3+ (a), Ge2+ (b) Sn4+ (c), and Er3+ (d) upon white light exposure, Figure S7: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Cu+ (a), Lu3+ (b) Mg2+ (c), and Gd3+ (d) upon white light exposure, Figure S8: The evolution of the UV-vis absorption spectra of Pb0.95M0.01/nI2, where Mn+ = Yb3+ (a) and Hg2+ (b) upon white light exposure, Figures S9–S11: The evolution of the XRD patterns of the Pb0.95M0.01/nI2 films after 400 h of light exposure, Figure S12: The photochemical aging dynamics of the Pb0.95M0.01/nI2 films represented by the evolution of the normalized film absorbance as a function of the aging time.

Author Contributions

M.I.U. carried out all experimental work on sample preparation, aging experiments, UV-Vis characterization, and analysis of the data. G.V.S. performed XRD measurements. L.A.F. contributed to conceptualization, visualization, and funding acquisition. S.M.A. contributed to project administration. P.A.T. contributed to experimental design, prepared the initial draft, and proofread the manuscript. All authors have read and agreed to the published version of the manuscript.

Funding

This work was supported by the Ministry of Science and Higher Education of the Russian Federation (Grant No. 13.2251.21.0163 (075-15-2022-1217)).

Data Availability Statement

The original contributions presented in this study are included in the article/Supplementary Material. Further inquiries can be directed to the corresponding authors.

Acknowledgments

The authors thank Denis V. Korchagin for recording some XRD patterns.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. The evolution of the UV-Vis absorption spectra of PbI2 (a) and Pb0.95Fe0.05I2 (b) films upon white light exposure. The survey of the aging behavior of different Pb0.95M0.1/nI2 films in terms of their normalized absorbance after 400 h of light exposure (c) and relative phase composition according to the XRD data (d).
Figure 1. The evolution of the UV-Vis absorption spectra of PbI2 (a) and Pb0.95Fe0.05I2 (b) films upon white light exposure. The survey of the aging behavior of different Pb0.95M0.1/nI2 films in terms of their normalized absorbance after 400 h of light exposure (c) and relative phase composition according to the XRD data (d).
Inorganics 13 00013 g001
Figure 2. The photochemical aging dynamics of the selected Pb0.95M0.1/nI2 films represented by the evolution of the normalized film absorbance as a function of the aging time (a). The dependencies corresponding to the first (b), second (c), and third (d)-order reaction kinetics are plotted in the corresponding linear coordinates.
Figure 2. The photochemical aging dynamics of the selected Pb0.95M0.1/nI2 films represented by the evolution of the normalized film absorbance as a function of the aging time (a). The dependencies corresponding to the first (b), second (c), and third (d)-order reaction kinetics are plotted in the corresponding linear coordinates.
Inorganics 13 00013 g002
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MDPI and ACS Style

Ustinova, M.I.; Shilov, G.V.; Troshin, P.A.; Aldoshin, S.M.; Frolova, L.A. Getting to the Heart of the Matter: Control over the Photolysis of PbI2 Through Partial Lead Substitution. Inorganics 2025, 13, 13. https://doi.org/10.3390/inorganics13010013

AMA Style

Ustinova MI, Shilov GV, Troshin PA, Aldoshin SM, Frolova LA. Getting to the Heart of the Matter: Control over the Photolysis of PbI2 Through Partial Lead Substitution. Inorganics. 2025; 13(1):13. https://doi.org/10.3390/inorganics13010013

Chicago/Turabian Style

Ustinova, Marina I., Gennadii V. Shilov, Pavel A. Troshin, Sergey M. Aldoshin, and Lyubov A. Frolova. 2025. "Getting to the Heart of the Matter: Control over the Photolysis of PbI2 Through Partial Lead Substitution" Inorganics 13, no. 1: 13. https://doi.org/10.3390/inorganics13010013

APA Style

Ustinova, M. I., Shilov, G. V., Troshin, P. A., Aldoshin, S. M., & Frolova, L. A. (2025). Getting to the Heart of the Matter: Control over the Photolysis of PbI2 Through Partial Lead Substitution. Inorganics, 13(1), 13. https://doi.org/10.3390/inorganics13010013

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