Methylammonium chloride was synthesized by countering 30 mL methylamine (40% mono, from Qualikems) and 20 mL hydrochloric acid (32% in water, from Merck). The three arms flask was filled with methylamine and HCl is added drop wise with methylamine solution at (8˚C - 10˚C) for 1 h with stirring. As synthesized methylammonium chloride was kept in ice for bath 3 hours. The precipitation was removed by putting the solution on a dry oven and carefully eliminating the solvent at 60˚C. The crystalline CH₃NH₃Cl was cleaned several times by diethyl ether (from Merck) and dried for 24 hours using dry oven at 60˚C. Then dried light yellow white powder of CH₃NH₃Cl was collected. Precursor 0.168 g of CH₃NH₃Cl was dissolved into 5 mL N, N-dimethylformamide and 0.564 g CuCl₂ was dissolved into 5 mL N, N- dimethylformamide (1:1) separately. Then light yellow solution of CH₃NH₃CuCl₃ perovskites was obtained. Graphene was prepared according to a modified Hummer’s Method and it was added at concentrations 0.05 g·ml⁻¹ at 45 mass% with pristine perovskite (Figure 2(b) and Figure 2(c)) solution to obtain G-MACuCl₃.

At low temperature TiO₂ solution was prepared using PEG (Polyethylene Glycol), Distilled water and TiO₂ respectively 1:20:3 ratio. PEG normally was used for better dispersion of solution to obtain uniform film [34]. The TiO₂ solution (3 mg/ml) was deposited on pre-cleaned ITO (ITO were cleaned by sequential 15 min sonication in warm distilled water, acetone and ethanol, pursued by drying in an oven at 60˚C) substrates by Dr. Blade method. Then it was positioned on a hot plate set to 40˚C for 10 min and at 70˚C for 10 min and we transferred to furnace for annealing at 350˚C for 20 min to improve the film stickiness. Then Perovskites (Pristine solution MACuCl₃, G-MACuCl₃) solution were deposited on TiO₂ film coated ITO using spin-coating method at 2000 rpm for 30 s [33] followed by heating at 80˚C for 15 min until crystal growth. Graphite layer was coated by candle on the another ITO as the hole transport materials (HTM). Then both ITO were sandwiched together using two binder clips (Figure 1(c)).

X-ray diffration (XRD) data were composed on GBC EMMA X-ray diffractometer

at Wazed Miah Science Research Center, Jahangirnagar University with Cu Kα radiation (λ = 1.54 Å). The scanning angular range was 5˚ ≤ 2θ ≤ 50˚ to get possible fundamental picks for each sample. UV-Vis spectrum of methylamine chloride, methylammonium copper chloride perovskite solution and methylammonium copper chloride graphene at 60˚C was studied using the UV-Vis Spectrophotometer Model: UVS-2800 at wavelength range of 190 nm - 1100 nm and very low stray light and noise specifications. The IR spectra of the samples were verified at room temperature using a SHIMADZU, IR Tracer-100, Japan. The wave number range was from 400 cm⁻¹ to 4000 cm⁻¹. The device performance was characterized without any encapsulation using solar simulator (IEC 60904-9 Edition2 and ASTM E927-10 standards, BCSIR, Bangladesh) under an AM1.5G filter at 100 mW/cm² in air and the intensity was standardized using a certified perovskite photodiode.

Before Figure 1(a) shows the XRD peaks of synthesized thin film Methylammonium copper chloride and graphene incorporated methylammonium copper chloride. Diffraction peaks at 9.38˚, 17.67˚, and 28.81˚ are indexed to be (001), (110), and (003) for CH₃NH₃CuCl₃ crystal planes, and other peaks are assigned to the glass substrate. For graphene assorted perovskite we observed new planes (111), (022) and (201) attributed at 20.53˚, 29.54˚ and 30.36˚ respectively in the XRD. In further we can progress crystalinity with the incorporation of graphene which was exposed by the intensity change in the (001) plane. We analyzed the crystallite size full and width half maxima (FWHM) for MACl, MACuCl₃ and G-MACuCl₃ viewed that the FWHM is smallest for G-MACuCl₃ demonstrating the highest crystallinity of the perovskite phase in the (001) plane attributed 9.38˚. However, the peak widths at half-maxima are about the same for both samples after normalizing the perovskite (001) peak intensities, denotation that on average, the differences in crystallinity are not significant. The average crystallites size were measured 43.015 nm for MACuCl₃ and 63.135 nm for Graphene-MACuCl₃ powder crystal (Figure 1(b)) which assembled uniformly due to sharp peaks achieved. The first order peak maxima synthesized thin film (001) for Methylammonium copper chloride and crystallite size also increased 180.44 nm and 200.56 nm respectively compare to the powder XRD reading and all are monoclinic lattice system. Volume of unit cell MACuCl₃ and graphene incorporated MACuCl₃ perovskite is 783(Å)³ and 1200.2(Å)³ respectively (Table 1). Thin film X-ray diffraction patterns of these two films are revealed in Figure 1(a) and compared to their respective powders. In both the cases, the (00l) reflections are finer [37], the annealing conditions were optimized to acquire crystalline, single-phase films.

There are several peaks of these three FTIR curves in the FTIR spectrum of MACuCl₃ and G-MACuCl₃ (Figure 2(b)) have a broad band at about 3510 cm⁻¹ which indicate the water bond O-H stretching which are not present in MACl. The second vibration mode 3052 cm⁻¹ of MACuCl₃ and 3050 cm⁻¹ for G-MACuCl₃ which indicates the alkanes groups of C-H stretching but this curve is smaller than MACl. The spectrum (black) represents the large cation salt methylammonium chloride. In this curve the bond C-H is stretching alkanes, C-N stretching amines, alkanes bending C-H and bending C-O are present [33] Similar vibration mode 1651 cm⁻¹ is attributed at both materials as synthesized MACuCl₃ and G-MACuCl₃ which is not found in MAI. The vibrational mode 1651 cm⁻¹ indicates the carbon-oxygen stretching [34].

On site Coulomb interactions with the DFT method together (U+DFT) was used to schoolwork the electronic structure of copper perovskite materials. These copper ions(Cu⁺) enclosing compounds illustrate the most unwavering ferromagnetic configuration within self-governing inorganic planes, while the interplanar

pairing is anti-ferromagnetic (AFM), corresponding with previous electronic and magnetic studies of (CH₃NH₃)₂CuCl₄ [38]. The absorption spectra of the series MACuCl₃ and G-MACuCl₃ show typical features improving absorbance [35] of graphene incorporated and highest absorption peak 341 nm and 243.25 nm respectively (Figure 3(a)). Strong bands for each material with coefficient absorption up to 200 cm⁻¹ are originated below 350 nm, and determined the corresponding band gaps from Tauc plots (Figure 3(c) and Figure 3(d)) are 2.60 eV (477 nm) for powder MACuCl₃, 2.61 eV (475 nm) for powder G-MACuCl₃, 2.61 eV (474 nm) for thin film MACuCl₃ and improved band gap 2.56 eV (483 nm) for thin film G-MACuCl₃ (Table 3). MACuCl₃ and G-MACuCl₃ were referred for future optimization by good feature of their better stability and improved optoelectronic properties, respectively [36]. ITO films acquired a high excellence transparent electrode which has been measured low resistance as per 10 Ω-cm and an elevated optical transmittance in the visible range by RF sputtering and premeditated their application as transparent electrodes in outsized area electric devices [39].

Multilayer films with high absorbance and visible transmittance below 20% were demonstrated as like ITO/TiO₂, ITO/TiO₂/MACuCl₃ and ITO/TiO₂G-MACuCl₃ by sputtering at room temperature and examined the electrical and optical

characteristics of multilayer structures and single-layer (Figure 4(a) and Figure 4(b)). Besides, the transmittance is found to be mainly reliant on the thickness of TiO₂ film. Based on Figure 4(b) it can be observed that multilayer ITO/TiO₂/MACuCl₃ and ITO/TiO₂G-MACuCl₃ films show higher absorbance than pure ITO film.

Current density-Voltage (J-V) curves were found after enlightening the CH₃NH₃CuCl₃ and Graphene-CH₃NH₃CuCl₃ solar cells under ambient condition. The undefended CH₃NH₃CuCl₃ cells illustrated a rapid decline in the short-circuit current and open circuit-voltage (Figure 5(c) and Figure 5(d)). After 40 days of revelation to moisture, photovoltaic behavior is investigated from the cells. Figure 5(a) and Figure 5(b) shows the J-V curves of CH₃NH₃CuCl₃ solar cells summarized with graphene composite. For graphene composition enhanced the stability of the cells to moisture. This explains why graphene composite demonstrate good stability in towering humidity conditions. The best performing cell with a self-protective coating confirmed a photocurrent of 0.21 mA·cm⁻² and an open-circuit voltage of 334 mV. The low open-circuit voltage found when compared to the best performing cell in literature deposited with graphite is due to the high recombination losses with CH₃NH₃CuCl₃ [39]. Changing graphene concentration that exhibits lower recombination sufferers than CH₃NH₃CuCl₃ and the performance of the photovoltaic device can be further optimized. Devices were fabricated with ITO/TiO₂/CH₃NH₃CuCl₃/graphite/ITO consuming graphite itself as the HTM established higher open-circuit voltage of 0.334 V, but lower short-circuit current density of 0.039 mA·cm⁻² (Table 4) due to low conductivity of graphene compared with CH₃NH₃CuCl₃ (Figure 5(c) and Figure 5(d)). Utilizing of more conductive materials further optimization, graphene can also progress the stability of the devices. Photocurrent vibrations is pragmatic in samples with copper based perovskites and with composition of graphene this could be due to the graphene incorporation performing as a buffer layer and avoiding the direct contact of TiO₂ and the graphite HTM [40]. The crystal size during the CH₃NH₃CuCl₃ growth is also another factor that can set in to the variation of photocurrents and therefore claims photocurrents decreasing with regards to the graphene incorporation. The shunt (R_SH) and series resistances (R_S) are considered to study the effect of graphene self-protective coating on the electrical

performance of the devices using the J-V data of the devices in Figure 5. The degradation of the perovskite due to the diffusion of oxygen and moisture into the perovskite layer was investigated. In spite of the shunt and series resistances of the cells, we look forward to the perovskite degradation machinery to be the identical. Therefore, the results of the achieved with higher series resistances and lower shunt (compared to best performing cells) could be unmitigated to high efficiency cells [40]. We finished a reference cell without protective coating and compared our power conversion efficiency to make sure suitable comparison.

The device without any graphene revealed a 15.5 KΩ of R_SH and a 2.4 KΩ of R_S. Where the device one with graphene composite illustrated a increase in both R_SH and R_S to a 61 KΩ and 29 KΩ respectively. Although the R_SH and R_S resistances are increasing with increase of graphene composition, but the ratio of R_SH/R_S has reduced from 6.45 to 2.11 for the devices without graphene and with graphene. Due to graphene incorporated into the perovskite a larger nanocomposite is fashioned which volume of unit cell increased 783 (Å)³ to 1200 (Å)³ (see Table 1) results in a augment in the R_S of the coated devices. Beside that holes of CuCl and the conduction band electrons of TiO₂ show the way to the lower shunt resistance(R_SH) due to CuCl may come in contact with the TiO₂ [41]. Low conductivity of without graphene compared to the graphene composite of perovskites because of reduce in the R_SH [42]. Figure 5(c) and Figure 5(d) showed using graphite as HTM and 8 μm TiO₂, solar cell devices were realized with MACuCl₃ and Graphene-MACuCl₃ characterized. MACuCl₃ consented a power conversion efficiency of 0.00152%, with V_oc = 334 mV, J_sc = 215 μA/cm², and FF = 42.82%. Graphene-MACuCl₃ gave a much lower power conversion efficiency of 0.00065%, though the optimized band gap (2.56 eV) less than MACuCl₃ and J_sc = 112 μA/cm², V_oc = 330 mV, and FF = 0.47 (Table 4). Because of Cu²⁺ reduction (as confirmed by XPS and photoluminescence measurements) the higher trap density commenced for lower performance of Graphene-MACuCl₃ which establish an additional way for charge recombination. To bear out the repairing behavior of the cell operating under dark condition (Figure 5(a)) the two devices was investigated in a wider range from −5V to +5V for dark current. High dark currents found (Figures 5(a)-(c)) at existence of high leakage current probably due to the direct make contact between the TiO₂ and graphite (HTM), assisted by the absence of perovskite checking layer over the TiO₂. Another limitation factor, band gap 2.61 eV and 2.56 eV suggesting deprived electron transfer in the device (Figure 3(d)) from ultraviolet photoelectron spectroscopy (UVS-2800) measurements. The devices based on MACuCl₃ and G-MACuCl₃ were demonstrated the sensitization action of the perovskite (see Figure 5(e)) in photocurrent measurements. The measurement was presented using Solar simulator (1.5 AM at 25˚C and power 1KW, BCSIR, Dhaka, Bangladesh). In précis, graphene composite has been found to perform as a multifunctional coating facilitating charge-carrier transport while simultaneously as long as an impervious seal to moisture [43], representing a corroboration of perception composite coating for superior photovoltaic stability [44]. The composite averts degradation of the CH₃NH₃CuCl₃ from UV, moisture, and air as revealed by the constant short circuit current density over an absolute period of time. The shielding graphene composite successfully checks the corrosion of the CH₃NH₃CuCl₃ into the Cl₂ and CuCl₂ [45]. The processing of CH₃NH₃CuCl₃ cells under atmospheric conditions once they are summarized with graphene composite which could allow the high moisture impermeability. In this work for both oxygen and moisture sensitive use of composite defensive materials could be comprehensive other lead free organic-inorganic metal halide perovskites. In this paper the sandwich approach could build up opportunities for coated or roll to roll perovskite cells and suggest important diminution in the processing costs. The use of coated counter electrode and the optimization of the composite for the cells continuing efforts engage fabrication of higher efficiency cells with graphite. It is currently followed using graphene with CH₃NH₃CuCl₃ crystals to prevent moisture from solar cells atmospheric roll to roll process is used. Similar perception can also be useful to design and widen different materials for lamination to grant long term stability.