Comparative Study on the Crystallite Size and Bandgap of Perovskite by Diverse Methods

Ahmed, Mohammad Tanvir; Islam, Shariful; Ahmed, Farid

doi:https://doi.org/10.1155/2022/9535932

Advances in Condensed Matter Physics

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Abstract Introduction Results and Discussion Conclusion Data Availability Conflicts of Interest Acknowledgments Supplementary Materials References Copyright Related Articles

Research Article | Open Access

Volume 2022 | Article ID 9535932 | https://doi.org/10.1155/2022/9535932

Comparative Study on the Crystallite Size and Bandgap of Perovskite by Diverse Methods

Mohammad Tanvir Ahmed,¹Shariful Islam,¹and Farid Ahmed¹

Academic Editor: Maheswar Nayak

Received21 Jan 2022

Revised24 Feb 2022

Accepted02 Apr 2022

Published17 May 2022

Abstract

This research demonstrates the fast synthesis of CH₃NH₃PbBr₃ perovskite powder via antisolvent addition and further thin-film synthesis by one-step spin coating. The structural and optical properties are investigated via X-ray diffraction, Fourier-transform infrared spectroscopy, and UV–Vis spectroscopy. Crystallite sizes are compared by three different size estimation techniques, which range between 95.8 nm and 105 nm. The perovskite showed a higher absorption coefficient over 10⁴ cm⁻¹ and a refractive index from 3.4 to 2.3 in the visible spectrum. The bandgap was estimated via three district methods, which revealed a very slightly varied bandgap in the range of 2.29 eV–2.32 eV.

1. Introduction

Organic-inorganic (OI) perovskites have become a common choice in the research of various optoelectronic (OE) fields. The general formula of OI perovskites is ABX₃, with A, B, and X representing organic cation, metal cation, and halide ion. The enhanced OE properties, abundance of materials, and easy synthesis process made ABX₃ very popular for numerous applications [1, 2]. OI perovskites have shown remarkable success in 3^rd generation photovoltaic research, attaining over 25.5% power conversion efficiency [3]. Perovskite materials can offer higher absorption coefficients, broader absorption spectra, higher carrier mobility, longer diffusive lengths, and tunable bandgaps [3]; hence, they are very potential materials for numerous OE applications.

Bromide and iodide-based perovskites are most popular due to their higher absorption coefficient and preferable bandgaps in the visible region. However, CH₃NH₃PbBr₃ perovskites are an outstanding compromise between the bandgap and better thermodynamic stability [4], which is an advantage in optoelectronic research over other OI perovskites.

Weber et al. successfully studied the different compositions of the three-dimensional CH₃NH₃PbX₃ perovskite material by modifying its crystal structure [5]. They have demonstrated three distinct phases of CH₃NH₃PbBr₃ (i.e., cubic, tetragonal, and orthorhombic) and the dependency of lattice parameters on temperature. Schmidt et al. synthesized nanosized CH₃NH₃PbBr₃ perovskites using NH₄Br, keeping the nanoparticles dispersed in various solvents [6]. The fast growth of perovskite crystals can be performed via the addition of the antisolvent with the precursor [7], which allows rapid growth of microcrystals or nanocrystals in a short time. Zheng et al. synthesized nanoplatelets of CH₃NH₃PbBr₃ using chlorobenzene as the antisolvent, which revealed a higher quantum yield of photoluminescence and a higher decay time [8].

Both the optical and electrical properties of materials are dependent on the synthesis method, the structure of the material, particle size, etc. The estimated particle size and bandgap also depend on the methods of calculation.

The most common method of perovskite synthesis is via evaporation of a precursor solution at low temperatures [9]. For thin-film preparation, various methods such as sol-gel spin coating, microwave-assisted methods, dip coating, spray pyrolysis, and physical vapour deposition have been developed [10]. Among them, the spin coating method is more desirable for perovskite film synthesis due to its high film coverage and low cost [11].

To estimate the average crystallite size from XRD, the Debye–Scherrer (DS) method, the Williamson–Hall (WH) method, and the Halder–Wagner (HW) method can be used [12]. Similarly, bandgaps can be studied via several methods, such as the Tauc method, the Kubelka−Munk (KM) relation, photoluminescence (PL) spectroscopy, and temperature-resistivity relation [13–17].

Here, we report the fast synthesis of methylamine lead bromide (MAPB) perovskites via the addition of the antisolvent. Structural, optical, and electrical properties of MAPB have been reported. A comparative study of the crystallite size and optical bandgap via different methods has also been performed.

2. Experimental Section

2.1. MAPB Synthesis

The materials used in the synthesis process of MAPB are methylamine (MA) solution 33 wt%, diethyl ether (DE), PbBr₂ 99%, hydrobromic acid (HBr) 48%, N,N dimethylformamide (DMF), and toluene.

MA and HBr were reacted at 1 : 1 molar ratio in an ice bath under the temperature of 0°C. After 20 minutes of stirring, the mixture was heated and white MABr crystals were obtained, which were washed several times with DE for removing impurities. MABr and PbBr₂ were dissolved in DMF at 1 : 1 ratio to prepare a 0.027 M MAPB solution. The pH and viscosity of the solution were about 5.6 and 1.35 mPa-s. The pH was measured as quickly as possible since DMF dissolves the plastic of the pH sensor. The solution was added dropwise in toluene with continuous stirring. The orange MAPB powder was precipitated, which was then collected via centrifugation. X-ray diffraction was immediately performed on the powder and, later, it was spin coated on a glass substrate for optical characterization. For electrical characterization, a thin disc of MAPB powder was prepared. Figure 1 shows the prepared MAPB powder and thin film.

2.2. Characterization

The X-ray diffraction (XRD) and Fourier-transform infrared (FTIR) spectroscopy analyses were performed for all the prepared samples via an Explorer diffractometer and IRPrestige-21, respectively. UV-Vis spectroscopy and Wayne Kerr 6500B Impedance Analyzer were used for analyzing optical and electrical properties.

3. Results and Discussion

3.1. XRD Analysis

The XRD peaks of the prepared MAPB powder were observed at 2θ values of 15.01°, 21.25°, 26.10°, 30.16°, 33.85°, 37.18°, and 43.19° (Figure 2), corresponding to (100), (110), (111), (200), (210), (211), and (220) planes, respectively [18]. The prepared MAPB powder showed fine crystallinity with high periodicity along the (100) direction. The MAPB powder was calculated to be in the cubic phase with a lattice parameter of a = 5.93076 Å. The average crystallite was calculated from the DS equation [19, 20]:where D_DS, k, λ, and Γ_s are the crystallite size, Scherrer constant (0.9), X-ray wavelength, and full-width half maxima, respectively. The average crystallite size obtained from the DS method is 95.8 nm. Williamson–Hall (WH) analysis is another simplified method to determine the average crystallite size from peak broadening [19]. According to the WH method, the X-ray diffraction peak widens due to the size and microstrain. The overall broadening may be expressed as follows:where D_WH and ξ are the average crystallite size (measured by WH method) and microstrain, respectively. The intercept of the 4 sinθ vs. Г_s cosθ plot (Figure 3) is used for D_WH estimation. On the other hand, according to the Halder–Wagner (HW) method, the relation between the microstrain, the crystallite size (D_HW), and Г_s can be written as

Hence, in this case, the slope of vs. plot (Figure 3) will determine D_HW. The average crystallite sizes obtained by DS, WH, and HW methods are 95.8 nm, 103.5 nm, and 105 nm, respectively.

3.2. Vibrational Modes

The FTIR spectra (Figure 4) of the MAPB perovskite show various modes of vibration present in MAPB. C-N stretching, C-H₃ bending, NH₃ bending, CH₃-NH₃ rocking, C-H stretching, and N-H stretching vibrations r identified from the peaks at 960 cm⁻¹, 1426 cm⁻¹, 1584 cm⁻¹, 1260 cm⁻¹, 2965 cm⁻¹, and 3131 cm⁻¹, respectively [21, 22]. However, no peaks of Pb-Br vibrations have been identified since PbX₂ is transparent in IR radiation [23]. The O-H stretching peak represents the presence of moisture in the MAPB sample.

3.3. Optical Properties

The absorbance (A) and reflectance (R) spectra of MAPB were studied in the wavelength range 400 nm–700 nm (Figure 5). The prepared MAPB sample showed higher absorption of the visible spectrum at a shorter wavelength range with an absorption peak at 523 nm [24]. The absorption spectrum shows a sharp absorption edge and very low absorbance in the longer wavelength region of the visible spectrum [4]. Higher reflectance, about 36%, was observed in the longer wavelength region, which signifies the percentage of incident energy loss via reflection. At lower wavelength, the reflectance is comparatively low. The variation of reflectance with the incident wavelength is quite similar to the previous report [25]. Due to low temperature (<150°C), MAPB possessed a higher structural disorder [4]; as a result, crystallite size reduced up to the nanoparticle dimension as obtained from the XRD analysis.

The absorption coefficient and skin depth can be calculated from the following equations [26]:where α, δ, A, and t represent absorption coefficient, skin depth, absorbance, and film thickness, respectively. Figure 6 shows that a of MAPB is the order of 10⁴ cm⁻¹, very preferable for OE applications. In the visible region, the absorption coefficient’s maximum value is about 2.33 × 10⁴ cm⁻¹, with an analogous skin depth of 0.04 μm, whereas at 700 nm, a is 0.26 × 10⁴ cm⁻¹ which corresponds to 0.364 μm skin depth. Hence, a few micron thick film is sufficient for absorbing most of the visible spectrum. The decrease in the crystallite size increases the dislocations; as a result, the percentage of voids increases. The increase in voids corresponds to a lower absorption coefficient, i.e., higher skin depth [27]. Hence, the skin depth can be reduced through increasing crystallinity.

The refractive index (η) and extinction coefficient (K) were obtained from the following set of equations [26]:where λ and R are the wavelength and reflectance, respectively; a higher refractive index corresponds to higher reflectivity, whereas the extinction coefficient (K) is the amount of light lost due to absorption or scattering per unit volume of a material. The material possesses a higher refractive index in the lower energy region and a higher extinction coefficient in the higher energy region of the visible spectrum. The maximum refractive index observed was around 2.2 eV energy, about 3.45 (Figure 7). The lower refractive index represents lower crystalline quality [28]. The refractive index can be increased to a higher value via increasing the crystallite size [27]. The peak of the extinction coefficient was near 2.37 eV. Since the extinction coefficient is proportional to the absorption coefficient, K can also be increased by increasing crystallinity.

The optical conductivity (OC) represents the rise in conduction electrons in the presence of photons. OC was calculated from the following equation [29]:where C represents the speed of light. Figure 8 shows that the OC of MAPB is very high in the higher energy regions with a strong peak at 2.37 eV and significantly lower in the low energy regions, which signifies the presence of higher electron density in the conduction band at higher energy absorption [29]. The OC is also a tunable property via maintaining the void percentage. An increase in voids can trap generated carriers. The overall optical conductivity of MAPB was very high, of the order of 10¹⁴ s⁻¹.

The direct bandgap (E_g) of MAPB was measured in both the Tauc method and KM method. From the Tauc method [30], where the bandgap is measured from the absorbance data, E_gA = 2.32 eV and, in the KM method, reflectance data were used to obtain the bandgap, which revealed E_gR = 2.29 eV (Figure 9). A slight variation was observed in the measured bandgap via different methods. The bandgaps are in good agreement with the previous report [27]. It is possible to tune the bandgap of MAPB via modifying the crystallite size since the nanoscale bandgap increases with decreasing crystallite size [31].

UV-Vis spectrometers usually generate absorbance (A) data from the transmittance (T) data through the Beer–Lambert law given by the following equation (7) [32]:

Although A + R+ T = 1 in theory, the spectrometer entirely ignores incident wave reflection when determining A. As a result, an exact value of absorbance cannot be achieved, resulting in some departure from correct readings.

On the other hand, the KM method for bandgap calculation holds good if the film is thick or shows poor absorption. Since the prepared film showed higher absorbance, the result shows a slight fluctuation and the obtained bandgap showed a certain deviation from the ones calculated via the earlier method.

3.4. Electrical Properties

The negative temperature coefficient of resistance (TCR) caused to decrease in the resistivity of MAPB with increasing temperature. The fitted plot showed an exponential variation of resistance of MAPB with temperature. According to the band theory of solids, the relation between temperature and resistance can be written as follows:where E_gE, k_B, T, and represent the energy gap between the top of the valance band and the bottom of the conduction band, Boltzmann constant, Kelvin temperature, and electrical resistance at temperature T, respectively. The above equation can be modified to

From the slope (13307.17) of the plot T ⁻¹ vs. ln(R) (Figure 10), the bandgap was calculated to be 2.296 eV, which is quite similar to the ones from previous methods. In the study, copper (Cu) metal was employed as the carrier conduction medium and electrodes. The resistance of Cu rose with temperature due to its metallic behavior, i.e., positive TCR, but the resistance of MAPI dropped with rising temperature. This phenomenon can generate an opposite effect on the carrier conduction through the system, causing a fluctuation in the resistance measurement, resulting in a bandgap deviation. The electrical resistance of the prepared sample depends on the crystallite/grain size. With decreasing crystallite size, the grain boundary per unit volume increases, which reduces the cross transport of charge carriers [33, 34]. Hence, the resistance increases with decreasing crystallinity.

4. Conclusion

The crystalline powder of MAPB perovskite was synthesized successfully via the addition of toluene as an antisolvent. The average crystallite size was calculated via three different methods from XRD spectra, and the obtained size ranged from 95.8 nm to 105 nm. The FTIR spectra verified the presence of different bonds in MAPB. The high absorption coefficient and optical conductivity of 10⁴ cm⁻¹ and 10¹⁴ s⁻¹ order were obtained, which are highly recommended for various OE applications. Up to 36% reflectance was observed with the refractive index from 3.45 to 2.3 in the visible wavelength region. The bandgap of the MAPB perovskite was measured via different methods (optical and electrical), and a very slight variation was observed. The measured bandgaps ranged from 2.29 eV to 2.32 eV.

Data Availability

The data used to support the findings of this study have not been made available because they are still being used in an ongoing research.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this article.

Acknowledgments

This research has been supported by the Condensed Matter Physics Lab of the Department of Physics, Jahangirnagar University, Dhaka-1342, Bangladesh. The financial support for this research was provided by the National Science and Technology (NST) fellowship under the Ministry of Science and Technology, Bangladesh.

Supplementary Materials

Graphical abstract of the research article. (Supplementary Materials)

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Copyright © 2022 Mohammad Tanvir Ahmed et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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