Investigation of the Stability of Methylammonium Lead Iodide (MAPbI3) Film Doped with Lead Cesium Triiodide (CsPbI3) Quantum Dots under an Oxygen Plasma Atmosphere.

In this study, we describe composited perovskite films based on the doping of lead cesium triiodide (CsPbI3) quantum dots (QDs) into methylammonium lead iodide (MAPbI3). CsPbI3 QDs and MAPbI3 were prepared by ligand-assisted re-precipitation and solution mixing, respectively. These films were optimized by oxygen plasma treatment, and the effect of powers from 0 to 80 W on the structural properties of the composited perovskite films is discussed. The experimental results showed that the light-harvesting ability of the films was enhanced at 20 W. The formation of the metastable state (lead(II) oxide and lead tetroxide) was demonstrated by peak differentiation-imitating. A low power enhanced the quality of the films due to the removal of organic impurities, whereas a high power caused surface damage in the films owing to the severe degradation of MAPbI3.

1. Introduction

Over the past several years, the study of inorganic halide perovskite as an optoelectronics material has gained significant consideration because of its extensive waveband (near-infrared) absorption and unique structural properties [1,2,3,4]. Quantum dots (QDs) display advantageous of optical and electrical properties [5,6] via the solution processing function. Therefore, turning inorganic halide perovskite into quantum dots by decreasing particle size to the nanoscale has become a dominant research subject in materials science, even at the commercialization stage. Meanwhile, promising applications in optoelectronics [7,8,9] also involve QDs due to their excellent photophysical properties. At present, the synthesis of QDs is based on various methods, including hot injection, ligand-assisted re-precipitation (LARP), ultrasonication, and solvothermal synthesis. Among these, the LARP method is superior to other methods in terms of the following characteristics: low cost, low processing temperature, simple equipment, and high processing rate. In 2016, supersaturated recrystallization (known as LARP) was firstly reported by Xiaoming Li [10]. It is operated at room temperature, occurs within few seconds, and does not require inert gas and injection. The authors utilized the X-type ligands oleic acid and oleoamine (OAm) to favor the formation of nanoparticles, but the stability of the product was poor and, as a consequence, it could not be modified, purified, and preserved for a long time. Besides, repeated purification or water treatment can easily lose the characteristics of PL [11,12,13]. Therefore, QDs were synthesizes with the L-type ligands, instead of the usual X-type ligands, by using OAm [14]. Although progress in the production of high-quality QDs has been made, practical applications of QDs are still a challenge. So far, the vast majority of scientists use hot injection, but this does involves a complex experimental process. Therefore, the LARP method to synthesize QDs with L-type ligands is preferred over other methods because it does not present the problems linked to X-type ligands. Current studies are mostly using lead (Pb), such as inorganic lead cesium triiodide (CsPbI3) and organic methylammonium lead iodide (MAPbI3) [1,2,3,4,5,6], due to its high stability and high performance resulting from interactions with organic and inorganic functional groups. The degradation of MAPbI3 is improved by doping the inorganic CsPbI3, inducing the break of MA bonding. The oxygen plasma treatment is also a common way to remove the organic contaminants onto the film surface and optimize the surface morphology. In addition, there are studies that mention that trace amounts of oxygen are beneficial to MAPbI3 films [15,16]. However, excess oxygen ions cause oxidation and ion bombardment [17], leading to a decrease of stability and a severe structural destruction of the film surface. In this article, we describe composite perovskite films based on doping of CsPbI3 QDs into MAPbI3. This innovative film, proposed as a potential material, is optimized by oxygen plasma treatment at different powers, and formation mechanism as well as its structural properties are investigated.

2. Results

The absorbance spectrum of composite perovskite films with MAPbI3 and CsPbI3 quantum dots (QDs) is shown in the wavelength range from 350 to 850 nm in Figure 1a. Compared to the pure MAPbI3 films, composited perovskite films demonstrate obvious absorption bands at 750 nm, proving that their light-harvesting ability in the long-wavelength range is enhanced by doping CsPbI3 QDs. The reason is that CsPbI3 QDs, a wide-energy gap material, show a small strain at the interface of CsPbI3 QDs and MAPbI3 [18,19], promoting film growth. Some related studies present the performance of photovoltaic devices, such as solar cells, which are improved after doping quantum dots into perovskite films [20,21]. The surface of composite perovskite films is further optimized via oxygen plasma treatment at different powers, from 20 to 80 W, as shown in Figure 1b. The strongest absorbance of the films was obtained at 20 W due to the removal of the excess impurities on their surface. With power in the range of 40 to 80 W, the absorbance gradually decreased owing to the degradation of MAPbI3 induced by the bombardment of oxygen ions at high power [17]. Another possible reason could be that the film surface suffered from the damage of oxygen ion bombardment, and this caused structure dispersion, similar to what observed in studies on plasma engineering [22]. Figure 1c shows the normalized photoluminescence (PL) spectra of the MAPbI3 films and composite perovskite films with and without oxygen plasma treatment at 20 W. It is observed that the luminous peak of the composite perovskite films presents an obvious red shift from 770.4 to 776.7 nm due to the doping of CsPbI3 QDs. In addition, the sample revealed an obvious blue shift to 773.2 nm after treating with oxygen plasma t 20 W, which may be attributed to the removal of the excess ligand and precursor. We also observed that, the intensity of these two samples was enhanced. These results were further proved by the crystallization measurement indicating variation of orientation.

Figure 1

Absorbance spectrum of (a) a MAPbI3 film with and without CsPbI3 QDs spin-coated onto glass substrate and (b) further optimization by oxygen plasma treatment from 0 to 80 W. (c) Normalized photoluminescence results of the MAPbI3 film and composite perovskite films with and without oxygen plasma treatment at 20 W.

Figure 2 demonstrates the X-ray diffraction (XRD) pattern of composite perovskite films composed of MAPbI3 and CsPbI3 QDs and treated with oxygen plasma at different powers, from 0 to 80 W. Based on the spectra of conventional MAPbI3 films [23,24], the peak position for MAPbI3 in composite perovskite films treated at 0, 20, and 40 W appeared at 14° and 28°. Compared to pure MAPbI3 films reported in other studies [23,24], the peak of PbI2 easily appeared in their XRD patterns, and PbI2 could cause a decrease of the absorption and the formation of defects in MAPbI3 films. This phenomenon was not found in our study. However, this phenomenon could be avoided by doping QDs in MAPbI3 film. The growth in the (001) orientation of PbI2 was not observed in the composite perovskite films. The doping of CsPbI3 QDs usefully inhibits the formation of PbI2 and even avoids the degradation of MAPbI3. This is due to the decrease of hydrogen bonding in MAPbI3 and the increase of octahedral tilting by the Cs ion exchange process [25,26]. When the power was higher than 60 W, the peaks of MAPbI3 at 14° and 28° disappeared, and then the (001) orientation of PbI2 emerged at the peak position of 12°. Generally, oxygen plasma treatment is used to remove impurities or organic materials from a film surface, thus improving it or optimizing the deposition frame. Excess ligand (oleylamine) and precursor (PbI2) were removed when the oxygen plasma power was below 20 W. At the power of 40 W, degradation of MAPbI3 occurred, and then PbI2 was successively produced. When the power increased to 60 and 80 W, oxygen ion bombardment caused severe structural damage or dispersion. This result is similar to those of other studies [17,22]. Thus, high-quality composite perovskite films can be prepared with lower oxygen plasma powers below 20 W.

Figure 2

XRD pattern of the composite perovskite films treated with oxygen plasma at various powers from 0 to 80 W.

As shown in Figure 3, the deconvolution results obtained at 0 and 20 W were analyzed by the peak differentiation-imitating to illustrate the proportion of CsPbI3 and MAPbI3 peaks which overlapped in the XRD pattern. The peaks of (I), (II), and (III) are represented in the (100) orientation of CsPbI3 at 13.97°, the (110) orientation of lead tetroxide (Pb3O4) at 14.05°, and the (110) orientation of MAPbI3 at 14.16°, respectively [27,28,29]. In Figure 3a,b, the peaks (III) and (I) are obviously the major and minor phases, respectively. The area ratios of the peaks (III) and (I) at 0 W were estimated at 85.7% and 8.3% and then varied to 64% and 9% at 20 W, respectively. Notably, when the power increased from 0 to 20 W, the Pb3O4 proportion dramatically increased from 5.8% to 26%, possibly due to the bonding of lead (Pb) in MAPbI3 with oxygen ions [30,31]. Meanwhile, these several oxygen ion species also bound to the carbon in MAPbI3, leading to the bonding of carbonyl groups (COX), as reported in other studies [32]. Furthermore, compared to the peak position of MAPbI3 films at (110) orientation, the composite perovskite films showed a peak shift of 0.02°, from 14.14° to 14.16°. This result indicated that the exchange of Cs ion to methylamine ion occurred in the MAPbI3 film with the increased oxygen plasma power, because the size of the Cs ion is smaller than that of the methylamine ion [33], leading to a decrease of the interplanar distance (d-spacing), from 3.153 to 3.148 Å. The d-spacing value (d) for the (110) orientation of MAPbI3 was calculated following Bragg equation [34]: where the n is the order of diffraction, λ is the wavelength of the X-ray sources, and θ as Bragg angle is the peak position of the (110) orientation of MAPbI3. On the other hand, in Figure 3c,d, the peaks of (IV) and (V) are represented in the (200) orientation of CsPbI3 at 28.4° and in the (220) orientation of MAPbI3 at 28.5°, respectively. Another shoulder peak of (VI) at (111) orientation at 28.54° is lead(II) oxide (PbO). The area ratio of the peak (VI) at 20 W decreased from 31% to 22%, mainly owing to the extra bonding of lead (Pb) in MAPbI3 with oxygen ions [31,35]. Figure 4 shows top-view SEM images of films treated with oxygen plasma at different powers to further analyze their crystalline growth. Island clusters with obvious grain boundaries are observed initially in Figure 4a. As shown in Figure 4b, when the power increased to 20 W, the oxygen ion induced a slight bombardment, causing blurred grain boundaries and fine pinholes on the surface of the films. The grown crystalline structure at 20 W was still clear, as shown by the enhanced peak intensities in the XRD results. At increased powers, from 40 to 80 W, cell-like perovskite (CLP) appeared, and the grain boundaries became undefined, as shown in Figure 4c–e. The CLP number also increased as the power increased; however, at a power higher than 60 W a clear break of CLP was observed, possibly due to the degradation of MAPbI3 induced by the excess oxygen ions, resulting in the swelling and destruction of the film surface associated with COX [30,35]. These results are similar to those of some studies in surface or interfacial engineering via plasma treatment within chemical vapor disposition and atomic layer deposition [36]. Notably, the influence of oxygen ion bombardment gradually increased with increased power. This was proved by the variation of the films’ thickness.

Figure 3

Deconvolution results of films treated at the powers of (a) 0 W and (b) 20 W in the range from 13.5° to 14.7° and at (c) 0 W and (d) 20 W in the range from 27.5° to 29.5° through the peak differentiation-imitating.

Figure 4

Top-view SEM images of perovskite films composed of MAPbI3 and CsPbI3 QDs treated at different oxygen plasma powers, from (a–e) 0–80 W.

In Figure 5, the thickness of the composite perovskite films is further illustrated at the increase of the oxygen plasma power to demonstrate the influence of oxygen ion bombardment. When the oxygen plasma power was at 0 and 20 W, the film thickness was consistently close to 330 nm. However, the thickness sharply decreased to 263 and 201 nm at 40 and 60 W and then reached the lowest value of 189.3 nm at 80 W. Generally, an increasing plasma power enhances ion bombardment, leading to severe surface damage of the film due to the degradation of MAPbI3. The decrease in the degradation rate was evidenced by the decrease of the variation of film thickness (from 20.30% to 6.06%), as shown by the SEM and XRD results. This decreased degradation was due to the saturation reaction of MAPbI3 and oxygen [30].

Figure 5

Thickness of perovskite films composed of MAPbI3 and CsPbI3 QDs after surface treatment at various oxygen plasma powers from 0 to 80 W.

3. Materials and Methods

3.1. CsPbI3 QDs Fabrication and Centrifugation

The precursor solution of quantum dots (QDs) was prepared by mixing 0.4 mmol lead iodide (PbI2) (Acros organic, 99%) and 0.4 mmol CsI (Alfa Aesar, 99.9%) in oleic amine (2.4 mL) and DMF (J.T. Baker, 99.5%, 10 mL) while continuously stirring for 10 s, as shown in Figure 6a. As shown in Figure 6b, this precursor solution (0.5 mL) was quickly added to toluene (J.T. Baker, 99.8%, 10 mL) while stirring to obtain the CsPbI3 QDs solution. After stirring for 10 s, the colloidal crude solution obtained was centrifuged at 11,000 rpm for 15 min at 10 °C. The precipitate was collected and then successively dispersed in hexane. The above process was repeated several times.

Figure 6

Schematic diagram of the composite perovskite preparation for (a) the precursor solution to obtain (b) the CsPbI3 quantum dots (QDs) solution via the ligand-assisted re-precipitation method (LARP) and (c) the MAPbI3 solution via solution mixing.

As shown in Figure 6c, CH3NH3I (198.75 mg) and PbI2 (576.25 mg) were added into the a mixture of 0.5 mL of sulfoxide (DMSO) and γ–butyrolactone (GBL, 0.5 mL, 1:1 ratio) to obtain the precursor solution [37]. Then, this precursor solution was stirred at 300 rpm for 24 h in a glove box to obtain the perovskite MAPbI3 solution.

3.2. Fabrication of Composite Perovskite Films

CH3NH3I (50 μL) and CsPbI3 (1 mg) were mixed and then spin-coated onto a glass substrate in two steps, at 1000 rpm for 10 s and 5000 rpm for 20 s. Toluene was dropped on the spinning film for 15 s during the second step. Hereafter, the sample was annealed at 90 °C for 15 min to obtain the composite perovskite films. This composite perovskite films were further enhanced by oxygen plasma treatment at different powers, from 0 to 80 W. The plasma measurement was carried out by RF excitation with a power source of 13.56 MHz (Plasma Etch PC-150 plasma etching/cleaning system).

3.3. Characteristics Measurement

The absorbance spectrum of the composited perovskite films was measured by ultraviolet/visible (UV/vis) absorption spectroscopy (HITACHI, U-3900). The X-ray diffraction (XRD) patterns of the films were recorded using a Bruker D8 Discover X-ray diffractmeter with Grazing Incidence X-Ray Diffraction (GIXRD). The top-view surface morphologies of the films were determined by field-emission scanning electron microscopy (FESEM, JEOL-6330). The thickness of the films was estimated by an Ellipsometer (J. A. Woolam/M2000-DI). Normalized photoluminescence (PL) was measured by iHR350.

4. Conclusions

In this article, composite perovskite films were successfully prepared by doping CsPbI3 QDs into MAPbI3. A significant increase in absorbance was obtained at a near-infrared wavelength of 750 nm owing to the doping of CsPbI3 QDs. The power of 20 W obviously enhanced the absorbance of the films, possibly owing to the bonding of lead (Pb) in MAPbI3 and oxygen ions. According to the SEM images, the surface morphology of the films at 20 W did not suffer excessive damage. However, high powers from 40 to 80 W not only increased ion bombardment causing surface damage of the films but also aggravated the degradation of MAPbI3. The proportions of MAPbI3, PbO, and Pb3O4 were further estimated by the peak differentiation-imitating of the XRD results to evaluate the structural properties. The dramatic decrease of MAPbI3 from 85.7% to 64% proved that the optimization of composite perovskite films was achieved at the oxygen plasma power of 20 W.