Potassium- and Rubidium-Passivated Alloyed Perovskite Films: Optoelectronic Properties and Moisture Stability.

Halide perovskites passivated with potassium or rubidium show superior photovoltaic device performance compared to unpassivated samples. However, it is unclear which passivation route is more effective for film stability. Here, we directly compare the optoelectronic properties and stability of thin films when passivating triple-cation perovskite films with potassium or rubidium species. The optoelectronic and chemical studies reveal that the alloyed perovskites are tolerant toward higher loadings of potassium than rubidium. Whereas potassium complexes with bromide from the perovskite precursor solution to form thin surface passivation layers, rubidium additives favor the formation of phase-segregated micron-sized rubidium halide crystals. This tolerance to higher loadings of potassium allows us to achieve superior luminescent properties with potassium passivation. We also find that exposure to a humid atmosphere drives phase segregation and grain coalescence for all compositions, with the rubidium-passivated sample showing the highest sensitivity to nonperovskite phase formation. Our work highlights the benefits but also the limitations of these passivation approaches in maximizing both optoelectronic properties and the stability of perovskite films.

Metal halide perovskite solar cells have recently emerged as one of the most promising candidates for low-cost thin-film photovoltaics (PVs),[1] having now reached power conversion efficiencies (PCEs) close to 23%,[2] making them comparable to commercialized thin-film counterparts.[3] The favorable intrinsic properties of these materials, including a strong absorption coefficient,[4] sharp band edges with low levels of disorder,[5] photon recycling capability,[6,7] and excellent charge transport characteristics,[8] render them excellent candidates for related optoelectronic applications such as solar cells,[2] light-emitting diodes,[9] and transistors.[10] The general formula for this class of materials is ABX3, consisting of at least one monovalent cation at the A-sites, (e.g., cesium, Cs; methylammonium (MA), CH3NH3; formamidinium (FA), CH3(NH2)2); a divalent metal at the B-sites (e.g., Pb, Sn); and a halide at the X-sites (e.g., Cl, Br, I, or mixtures thereof). There has been intensive research on the addition of monovalent cations and halides into the perovskite precursor solutions to enhance the crystallinity,[11] phase stability,[12] and optoelectronic properties of the perovskite materials.[13,14] In particular, an alloyed perovskite such as (Cs0.06MA0.15FA0.79)Pb(I0.85Br0.15)3 (triple cation or TC) shows superior PV performance and moisture stability compared to a single-cation composition such as MAPbI3 and as a result has become one of the state-of-the-art perovskite compositions.[15−18] Recently, the addition of rubidium (Rb) halide into the TC perovskite has led to further enhanced performance and stability of perovskite solar cells, with an optimal loading for performance at 5% Rb with respect to the other A-site cations.[19,20] Furthermore, we and others have recently shown that passivation of TC films with potassium (K) halides can also significantly enhance the optoelectronic properties of perovskite device structures, with photoluminescence quantum efficiencies of ∼15% in complete solar cell stacks and the inhibition of photoinduced ion migration processes across a wide range of perovskite bandgaps.[21−24] We found that the optimal loading of K for achieving both high luminescence yield and excellent charge carrier transport is 10% K relative to the A-site cation.[25] The precise location of the passivating ions is still an open question in the community: recent evidence from the literature and our own work suggests that neither K nor Rb are incorporated within the perovskite lattice,[25,26] though there is also evidence that these ions may occupy interstitial sites[24] at the surfaces.[25] Despite the apparent similarities between the passivation routes of the TC films with Rb or K, a direct comparison between the two in terms of tolerance to loading fractions, overall effectiveness, and the viability of these approaches for stable perovskite thin films has not yet been performed.

Here, we directly compare the optoelectronic properties and chemical and structural stability of TC films passivated with Rb or K additives. We find that the TC films can incorporate higher loadings of K than Rb before undergoing large-scale phase segregation at larger loading fractions, an observation that correlates with K-passivated films with optimal loading levels exhibiting superior optoelectronic properties (such as luminescence efficiency) over Rb-passivated films. We find that both passivation routes lead to the formation of nonperovskite phases; for K, these phases selectively decorate the GBs and interfaces even up to high loadings (∼10%), while for Rb above ∼5% loading, the majority of the Rb is locked into large micron-sized nonperovskite crystallites. We track the structural, chemical, and morphological changes of these perovskites over time under humid conditions. We find superior moisture stability in ambient conditions for K-passivated TC films compared to Rb-passivated films, though in both cases over extended aging times and elevated humidity levels nonperovskite phases form. Interestingly, we also observe a substantial grain coalescence concomitant with further enhancement in the luminescence quantum yield for the TC and K-passivated samples under humid conditions. Our work reveals critical insight into the behavior and stability of passivation treatments on perovskite compositions, revealing key benefits and shortfalls of each approach.

We spin-coated a series of perovskite thin films on glass by diluting the concentration of the A-site cations in the TC precursor solutions with KI- and RbI-based solutions in different volume ratios (see the Methods section in the Supporting Information (SI)).[19,25,27] We denote the resulting passivated samples as x = [K or Rb]/([K or Rb] + [A]), where A = (Cs, FA, MA) and x represents the fraction of K or Rb out of the A-site cations in the precursor solution. In Figure a, we show the photoluminescence quantum efficiency (PLQE) of the (Cs0.06MA0.15FA0.79)Pb(I0.85Br0.15)3 perovskite films with increasing K and Rb content measured at excitation densities equivalent to 1 sun solar illumination conditions. We observe a large increase from the initial value of 18% for TC to 41% for K-passivated TC (x = 0.05), which increases further to 52% for x = 0.20.[25] However, we do not find an appreciable increase in the PLQE in the Rb-passivated samples beyond x = 0.05. We find that the loadings of K or Rb for peak solar cell device performance match those from luminescence, with the open-circuit voltage Voc (Figure b) and short-circuit current Jsc(Figure c) maximized at x = 0.05 for Rb-passivated TC devices but at x = 0.10 for K-passivated TC devices (see Figure S1 and Table S1 for current–voltage (J–V) curves and device parameters, respectively). The decrease at very high loadings is consistent with an increasing concentration of nonperovskite precipitates.[18] These results show that we can achieve superior optoelectronic properties through passivation with K than that with Rb; the K route offers greater versatility because wider ranges of loadings are possible before detrimental effects on performance parameters are observed.

Figure 1

(a) PLQE of passivated perovskite thin films measured under illumination with a 532 nm laser at an excitation intensity equivalent to ∼1 sun (∼60 mW·cm–2). (b) Open-circuit voltage (Voc) and (c) short-circuit current (Jsc) extracted from current–voltage characteristics of pristine and passivated TC perovskite devices measured under full simulated solar illumination conditions (AM1.5, 100 mW·cm–2) (see Figure S1 for J–V curves).

To investigate the local chemical and morphological composition of the passivated TC perovskite thin films, we performed scanning transmission electron microscopy energy dispersive X-ray spectroscopy (STEM-EDX) measurements. We prepared a lamella of the x = 0.10 sample for both K- and Rb-passivated TC perovskite films with 2,2′,7,7′-tetrakis(N,N-di-p-methoxyphenyl-amine)9,9′-spirobifluorene (Spiro-OMeTAD) and platinum capping layers to preserve the active layer during specimen preparation (see Figure a,d and Figure S2 for STEM high-angle annular dark field (HAADF) cross-sectional images). We used experimental parameters similar to those in our previous reports for different perovskite compositions in which we optimized the beam conditions to minimize any potential beam-induced damage or phase segregation.[28] We used a Non-negative Matrix Factorization (NMF) algorithm[29] to decompose different phases in the cross-sectional STEM-EDX of the thin films. This analysis reveals the presence of two different compositional phases in both K- and Rb-passivated TC samples, namely, a perovskite phase (identified from Br Lα, Pb Mα, and I Lα lines) and an additive-rich phase (Figure b,c,e,f; see Figures S3 and S4 for complete NMF decomposition results and Figures S5 and S6 for perovskite phases). In the K-passivated TC, we found that most of the K-(additive)-rich phase is composed of K and Br and situated at the grain boundaries (GBs) and interfaces of the perovskite film (Figure b), as we observed previously at higher loadings.[25] However, in the Rb-passivated TC at the same loading as the K sample, we observed that the majority of the Rb is contained in large, micron-sized crystals rich in Rb and I (Figure d–f) with no evidence for the presence of Rb selectively moving to the surfaces of the film within our experimental resolution (estimated to be ∼1 atom %). Complementary photoelectron spectroscopy (PES) measurements on the samples reveal that Rb is more uniformly distributed throughout the film, with a negligible change when probing the surface (XPS) and probing deeper into the bulk (via the use of hard X-rays, HAXPES); on the other hand, the K content is higher on the surface than that in the bulk (Figures g,h and S7). We note that we also did not observe any significant changes in binding energy within experimental resolution of the lead (Pb 4f) or halide (I 3d and Br 3d) core levels, consistent with these additives not incorporating into the perovskite lattice[21,30] (Figure S8). These results highlight an important finding: in the K-passivated samples, the K (even when added as KI) complexes selectively with the Br present in the TC precursor solution with an almost 1:1 atomic percent ratio, while the Rb interacts primarily with iodide with an atomic percent ratio of 1:2, with only smaller fractions of Br (I:Br ≈ 8; see Table S2 for atomic percent analyses from the STEM-EDX analyses). These results are consistent with a larger red shift of the PL peaks for K than that for Rb at the same loading of each due to a lower fraction of Br incorporated into the final perovskite lattice for K than that for Rb (Figure S9). These differences are also consistent with the lower formation energies of bonds comprising KBr and RbI relative to KI and RbBr, respectively.[31,32]

Figure 2

(a) HAADF STEM cross-sectional image of a TC perovskite thin film passivated with K (x = 0.10). (b) NMF decomposition of the K-passivated TC sample showing the KBr phase and (c) the corresponding EDX spectra (see Figure S5 for the perovskite phase). (d) HAADF STEM cross-sectional image of a TC perovskite thin film passivated with Rb (x = 0.10). (e) NMF decomposition of the Rb-passivated TC sample showing the Rb–I–Br phase and (f) the corresponding EDX spectra (see Figures S5 and S6 for the perovskite phase). Intensity ratios between different core levels of the (g) K and (h) Rb additives with respect to the lead with different probe beam energies from XPS (1486.6 eV) and HAXPES (4000 eV) measurements. We used Pb 4f, K 2p, Cs 4d, and Rb 3d core levels for all beam energies (see Figures S7 and S8 for full spectra).

In our previous work, we proposed that the K selectively draws the Br out from the lattice in the precursor solution. This allows exploitation of the beneficial effects of Br in the seeding of high-quality grain growth but then the removal of a fraction of the Br from the lattice of the final film, which would otherwise negatively impact optoelectronic properties.[33] By contrast, the Rb binds the iodide more strongly, but we do not see the same effects. Furthermore, the inferior solubility of RbI compared to that of KBr in the dimethylformamide (DMF)/dimethyl sulfoxide (DMSO) precursor solution[31,32] means that Rb precipitates into large Rb halide crystals at a lower loading than KBr, with the K-passivated samples primarily showing GB and surface decoration with the KBr species. These results provide an explanation for the superior optoelectronic properties of the K passivation route over Rb passivation: the greater solubility of the key nonperovskite phase in the former (KBr) compared to the latter (Rb–I–Br-based phase) means that the system is tolerant to a higher loading of beneficial passivating species of K than Rb, and the specificity of K for Br also contributes to the particularly large enhancements.

We then compared the atmospheric stability of the passivated films in each case, with the passivated samples fixed herein at x = 0.05 to ensure reasonable optoelectronic properties for both Rb and K. In Figure , we show top-view scanning electron microscopy (SEM) images of perovskite thin films exposed to ambient air (30% relative humidity, RH) for 1 week in dark conditions. We observe that the TC and K-passivated TC films remain unchanged, while needle-like crystals, distributed homogeneously across the sample area, form in the Rb-passivated TC films. Recent work suggests that these crystals are Rb-rich and that humidity accelerates their formation;[18] these crystals are likely to be similar species to those that we observe distributed more sparsely in the films with higher Rb loadings without humidity exposure (x = 0.10, Figure d–f). The formation of crystallites in the Rb samples but not in the K (or TC) samples can be attributed to the higher solubility of RbI at room temperature in water (1.69 g/mL) compared to KBr (0.681 g/mL).[31,32]

Figure 3

SEM top-view images at different magnifications of (a) TC, (b) Rb-passivated TC, and (c) K-passivated TC films prepared on glass/FTO/TiO2, with the images acquired after storage of the films in ambient laboratory air (30% RH) for 1 week in the dark.

In order to further investigate the moisture stability and the local chemistry of the passivated TC perovskite thin films, we stored the films under elevated humidity conditions (50% RH, N2) for a period of 24 h. In Figure , we show the morphology of the TC and Rb- and K-passivated TC perovskite films before (Figure a–c) and after (Figure d–f) this humidity treatment. We observed uniformly packed grains each of size ∼200–400 nm for all of the unexposed perovskite films (Figure a–c). However, following humidity exposure for 24 h, we observed the formation of material on the surfaces of all films. We propose that the surface material for the TC specimen corresponds primarily to PbI2 (cf. X-ray diffraction studies below), which is particularly abundant at the GBs (Figure d,g). This is similar to degradation in other polycrystalline materials where GBs are centers for degradation, often called intergranular degradation.[34] We also found sparsely spaced long needle-like crystals (≥30 μm) that, based on SEM-EDX analyses (Figures S10 and S11), are rich in Cs. Furthermore, we again observed the formation of Rb-rich crystals in Rb-passivated TCs, which appear to be primarily rich in I but also smaller fractions of Br (Figure e, h). Finally, we also observed the formation of KBr-rich surface crystallites in the K-passivated TC films after the humidity treatment, which have similar composition as those in our cross-sectional STEM-EDX decomposition profile but are of larger size and distributed across the surface. These results suggest that moderate humidity exposure promotes the formation of nonperovskite material in each of the film compositions, with the composition of the nonperovskite material being consistent with that observed at elevated loadings of additives.

Figure 4

Top-view SEM images of pristine (top row) and humidity-treated (50% RH, N2 over a course of 24 h; second row) (a,d) TC, (b,e) Rb-passivated TC, and (c,f) K-passivated TC perovskite thin films. SEM-EDX elemental maps of the same (g) TC, (h) Rb-passivated TC, and (i) K-passivated TC perovskite films.

Interestingly, we observe a significant coalescence of small perovskite grains into larger “fused” domains in the perovskite thin films upon 50% RH treatment in the TC and K-passivated TC (Figure a,d and c,f). We find that the average grain size increases remarkably from ∼200 nm to ∼2 μm in both samples (see Figure S12 for grain size distributions). Curiously, the perovskite grains in Rb-passivated TCs preserve their original average grain size distribution (Figure S12), though we note that under more extreme humidity conditions (i.e., 75% RH), we also see the coalescence in the Rb-passivated TCs (Figure S13). This suggests that the Rb-passivated TC perovskite films are more resistant to grain reconstruction.

In Table , we show the PLQE of the perovskite thin films before and after storage in a moderately humid environment (50% RH, N2). We observe significant enhancement in the radiative efficiency of the perovskite films for TC and K-passivated TC, with the PLQE increasing from 18.6 and 39.5%, respectively, to 27.9 and 49.2%, respectively. In contrast, the PLQE of Rb-passivated TC drops from 22.8 to 12.9% after exposure. We therefore find that the PLQE trend mirrors the grain fusing phenomena as the radiative efficiency of the humidity-treated TC and K-passivated sample with substantial grain coalescence increases substantially. This observation is consistent with previous reports showing that crystal (grain) coalescence is observed concomitant with enhanced optoelectronic properties of MAPbI3 perovskite thin films and the PV performance of the subsequent devices,[35,36] but to the best of our knowledge, this is the first time that this has been observed in the alloyed perovskite structures. We note that the positive impact on the PLQE of the grain coalescence in these samples must outweigh any negative effects induced by the observed crystallites on the surface (Figure g(i), which are in any case comprised of large bandgap material that will not quench luminescence and may in fact also further passivate (cf. PbI2).[37] We and others have also previously reported enhancements in MAPbI3 device performance with controlled exposure to humidity but did not observe grain coalescence in these cases.[38,39] We speculate that the drop in PLQE of the Rb-passivated TC films can be attributed to degradation of the perovskite to nonperovskite Rb-rich phases but without any beneficial grain coalescence. This is consistent with the reported drop in performance of the similarly treated Rb-passivated TC-based perovskite solar cells.[18] We note that the surface crystallites in the K and TC samples may still negatively influence interfacial charge collection. Furthermore, it is likely that any residual moisture will need to be removed, for example, through thermal annealing post-treatments, to prevent long-term degradation issues for ultimate device utilization. Thus, future work will be required to implement the samples with coalesced grains into full, optimized devices.

Table 1

PLQE of the Perovskite Thin Films Measured before and after Storage in Humid Nitrogen (50% RH) for 24 ha

	PLQE (%)
sample	before	after
TC	18.6	27.9
Rb-passivated TC	22.8	12.9
K-passivated TC	39.5	49.6

Films were illuminated with a 532 nm laser at an excitation intensity equivalent to 1 sun (∼60 mW·cm–2).

To further explore the structural stability of the perovskite thin films and to track the growth of perovskite and nonperovskite crystals upon humidity exposure, we performed XRD measurements on pristine films that were aged in humid nitrogen (50% RH) over the course of 1 day (Figures and S14). For the TC film, we observed a PbI2 peak (2θ = 12.7°) that becomes narrower and more intense with extended aging (Figure a), consistent with the formation of larger PbI2 crystallites at the perovskite surfaces and GBs (cf. Figure d). The humidity exposure also leads to the emergence of new reflections with peaks at 2θ = 10.0 and 11.2° that we assign to the yellow δ-phase of Cs-rich (Cs,FA,MA)(I0.85Br0.15)3[40] and CsPb2I4Br,[18] respectively, in agreement with the segregation of highly crystalline Cs-rich phases observed in the SEM-EDX analyses (Figures S10 and S11). For the pristine Rb-passivated perovskite (Figure b), we found a diffraction peak at 2θ = 9.9° that we tentatively ascribe either to the Rb-based perovskite RbPb(I0.85Br0.15)3[18] or to the yellow δ-phase of Cs-rich (Cs,FA,MA)(I0.85Br0.15)3[40] (as for the TC sample). During humidity exposure, this feature remains stable, but after 24 h, we also see the emergence of two new peaks at 2θ = 11.4 and 12.3° that we attribute to a segregated RbPb2I4Br phase.[18] In Figure c, it is evident that similar PbI2 and CsPb2I4Br reflections are present in the XRD data for the K-passivated TC sample albeit at much weaker intensities compared to the TC films. The XRD pattern corresponding to the K-passivated samples exposed for 24 h also contains a weak reflection at 2θ = 8.9° that may correspond to a hydrated lead-passivated K bromide compound (e.g., KPbBr3·H20),[41] with the SEM-EDX showing the presence of K- and Br-rich needle-like crystals on the sample surface (Figure c); a precise chemical identification is not possible at this stage.[42]

Figure 5

XRD patterns of (a) TC, (b) Rb-passivated TC, and (c) K-passivated TC perovskite thin films on glass exposed to humid nitrogen (50% RH) for the stated times. The features are assigned as stated; we assign the feature marked * to be the yellow δ-phase of Cs-rich (Cs,FA,MA)(I0.85Br0.15)3. (d) Peak position, (e) FWHM, and (f) peak area for the perovskite thin films over time.

In Figure d–f, we analyze the changes in the primary perovskite peak at 2θ ≈ 14.1° (Figure d), the full width at half-maximum (FWHM) (Figure e), and the peak area (Figure f) for the films at different exposure times. We observe that for both Rb- and K-passivated TC films, the perovskite peak is shifted toward lower angles relative to the peak from the TC sample, which indicates expansion of the perovskite lattice and is in agreement with previous reports.[18,25] This could be due to partial extraction of bromide from the perovskite lattice by the passivating additives or to the passivating species occupying interstitial sites. We note that we have not seen any significant trend on the perovskite peak position upon humidity treatment, suggesting that these effects are not further affected by humidity exposure. We find that the FWHM drops significantly and the peak intensity (area) increases upon humidity treatment for the TC and K-passivated TC perovskite films, which is in agreement with the grain coalescence that we reported earlier (Figure ). By contrast, these parameters remain similar for the Rb-passivated TC after humidity exposure in which the grain sizes remain similar.

In conclusion, we investigated the optoelectronic properties and chemical stability of state-of-the-art TC perovskite films passivated with K and Rb halides. We found that the luminescence efficiency increases to higher levels with K than that with Rb owing to the tolerance of the TC perovskites for higher loadings of K than Rb. We found that K selectively binds to bromide and Rb to iodide, and the increased tolerance of the perovskites to K over Rb is dictated by the enhanced solubility of KBr over Rb halides in the precursor solvents (i.e., DMF/DMSO).[31,32] At loadings above 5% Rb, large Rb halide-rich crystals form that negatively impact the performance, while K-based films retain their optimal performance even at 10% loading. We also observe that this unwanted crystal formation is exaggerated when exposed to humidity. At low humidity levels (∼30%), the Rb-rich phases form while the pristine and K-passivated TC perovskite films remain unaffected; this is attributed to the greater solubility of Rb halides in water over KBr and PbI2. Under higher humidity conditions (∼50%), we detect the appearance of PbI2 at the GBs and Cs-rich crystals for the TC films, segregation of Rb-rich phases in Rb-passivated TC films, and formation of a K-bromide phase in the K-passivated TC films. Interestingly, we found significant grain coalescence in the TC and K-passivated TC samples upon humidity treatment that further enhances the radiative efficiency of the perovskite thin films.

These results represent an important advance in understanding the local chemistry and the structural stability of the state-of-the-art perovskite thin films to push optoelectronic devices to their efficiency limits. Our work highlights the benefits but also the deficiencies of these passivation approaches. We speculate that the primary role of these additives is to manage halides and vacancies, but the resulting K- or Rb-rich species that immobilize the unwanted excess halide yet are redundant after processing (albeit electrically benign) may even compromise humidity stability. Future efforts should consider facile post-treatment processes to remove the additives after their role in film formation and passivation is complete, as well as novel approaches to exploit the grain coalescence to maximize optoelectronic properties such as luminescence and charge collection in full device structures.