The Effect of Indium Tin Oxide Nanoparticles (ITO NPs) Incorporated with ZnO NPs based on Structural, Optical and Flexible Dye Sensitized Solar Cells (FDSSCs) Application

1. Introduction

Flexible dye sensitized solar cells (FDSSCs) are a potentially more economical, clean, efficient, easy-to-fabricate, and environmentally friendly photovoltaic (PV) technology than traditional silicon-based ones [1,2]. It may also be used as flexible window or wall devices in building-integrated photovoltaic systems [3]. The majority of FDSSCs are composed of dye and semiconductor oxides. Numerous semiconductor oxides, including SnO₂, TiO₂, ZnO, and Nb₂O₅, have been used as an electron transport medium. Because of its special qualities, which include low cost, non-toxicity, and ease of synthesis, ZnO has proven to be an effective substitute for FDSSCs. Globally, nanotechnology is becoming more and more popular, finding utilizations in food, feed, pharmaceuticals, and personal hygiene products. [4] Nanoparticles are produced in comparatively high quantities using conventional procedures. [5] Due to their distinct characteristics, such particles have generated a lot of curiosity [6]. Nanoscale semiconductor materials [7] have novel properties because the quantum size effect or enormous surface area modifies their physical and chemical characteristics [8,9]. Of all the metal oxide nanomaterials currently accessible [9], zinc oxide Nanoparticles (ZnO NPs) [10] is an important material for research in a variety of applications. ZnO NPs hexagonal wurtzite structure [10] has garnered prominence as a luminescent material due to its structural [11], optical [12,13], thermal [13], electrical, and luminescence capabilities that can be used to make useful devices [14]. As nanomaterials’ shape, size, and distribution-dependent capabilities, structure [13,15], or morphology [10,13] management, ZnO NPs have long been a priority in nano research [16]. ZnO NPs are useful because it is non-toxic to the environment [17] and can withstand radiation. The features of ZnO NPs materials are known to be affected by the production method, growth conditions, and post-growth treatments [18]. To prepare the ZnO nanostructure [19], lots of methodologies have been adopted. Epitaxy, pulsed laser deposition, thermal evaporations, solvothermal method, vapor phase production [20], precipitation, sol-gel, and sonochemical method are just few of the methods used to create ZnO nanostructures [20,21].

Of all the methods mentioned above, sol-gel is an excellent choice for producing ZnO NPs [22] due to its ease of modification and affordability [23]. The use of this process for nanoparticle production offers several advantages, including shorter production times and lower operating temperatures compared to alternative methods. [24] The effect of annealing, ZnO NPs generated using the sol-gel technique was reported by Omri et al. [25] To investigate the formation of ZnO nanostructures, Kumar et al. [26] employed a sol-gel method involving zinc sulfate heptahydrate and NaOH as precursors. It was found that the bandgap of ZnO nanostructures can be lowered by increasing the calcination temperature, which in turn causes the maximum absorption to move to longer wavelengths. [25] The electrical and optical characteristics are highly correlated with the crystallite size and orientation, which are mostly influenced by the sizes of the NPs. There are still several challenges that must be overcome before effective ZnO NPs can be created. The first issue is characterizing the residual n-type conductivity of ZnO NPs that have been inadvertently doped. [27] Differences in hole concentrations and carrier mobility resulting from inconsistent doping types hinder the commercialization of ZnO homojunction systems. [28]

The most commonly used plastic substrates for conductive polymer substrates in DSSCs are polyethylene terephthalate (PET) and polyethylene naphthalate (PEN). Recently, coated ITO has also been added to both substrates. However, before using the non-flexible material in DSSCs, the anode and cathode films are heated for 30 minutes at 450 °C to eliminate any residues and solvents from the precursor. Fortunately, the thermal stability of PET and PEN polymer substrates is determined by the maximum temperatures used during processing. This means that if the maximum temperature of 150 °C is exceeded, the flexible electrode (ITO/PEN and ITO/PET substrate) may deform. It is therefore recommended to treat the polymer substrate at a temperature no higher than 150 °C. Unfortunately, due to the low-temperature treatment (low annealing) of the polymer substrate, which hampers efficient decomposition of precursor residues, the performance of DSSCs was poor.

In this study, we developed composite materials by combining ZnO nanoparticles (NPs) with ITO NPs. The purpose of this was to improve the power conversion efficiency (PCE) of ZnO NPs in FDSSCs, and to evaluate the impact of ITO NPs on ZnO NPs FDSSCs. To optimize the efficiency of the composites for FDSSCs, which were fabricated using di-tetrabutylammonium cis-bis-(isothiocyanato) bis (2,2′-bipyridyl-4,4′-dicarboxylato) ruthenium (II) (N719) dyes as sensitizers, we subsequently created composites of ITO NPs with ZnO NPs under appropriate conditions. This makes ITO NPs a potentially cost-effective addition. Metal oxide hybrids incorporating ITO NPs are appealing due to their ability to exhibit good optical performance (fluorescence emission) and their wide range of applications. Consequently, the addition of ITO NPs is advantageous for metal oxides. This perspective suggests that ITO NPs can enhance electron transport and reduce charge recombination by functioning as energy donors. The objective of this research is to modify the structure and optical properties of ZnO NPs, as well as improve FDSSCs performance, through hybridization with ITO NPs. We examined the formation of a ZnO NPs/ITO NPs hybrid connection and its impact on the composite. For ZnO NPs, we investigated the effect of ITO NPs on their structure, optical properties, and performance in FDSSCs.

2. Experimental Part

2.1. Reagents

From Across Organic, we obtained zinc acetate dehydrate (Zn (CH₃COO) ₂. 2H2O), sodium hydroxide (NaOH, 99%), indium (III) chloride (InCl₃. 4H₂O), tin (IV) chloride (SnCl₄. 5H2O), ethylenediamine (EDA) (99%), ammonium hydroxide (NH3) solution, acetonitrile (99.5%), and ethyl alcohol (99.5%)

2.2. (A) Synthesized of ZnO NPs and ZnO NPS composite with ITO NPs

0.1 M of zinc acetate dehydrate (Zn (CH₃COO)₂.2H₂O (99%) and 0.2 M of Sodium hydroxide (NaOH) dissolved separately in DI water (1:1 ratio Zn (CH₃COO).2H₂O: NaOH). Then NaOH added to Zn (CH₃COO)₂.2H₂O slowly dropwise vigorously stirring at room temperature. Then waiting up to a white transparent solution is formed. After the white transparent ZnO precipitate was formed, insert it in an oven at 80⁰C for 2hrs [29]. Centrifuge for 30 min at 3000rpm using ethanol and DI water. Then calcined at 300⁰C-500⁰C. Then using the sol-gel method ZnO NPs were prepared successfully.

2.2. (B) Preparation of ITO Nanoparticles by Sol-Gel Method

Indium(III) chloride (InCl₃. 4H₂O (2.6 g, 6.7 mmol) and Tin (IV) chloride (SnCl₄. 5H₂O (0.26 g, 0.74 mmol) was dissolved in 40 ^oC - 50 ^oC distilled water (10 mL) and the solution was stirred for 30 min. To regulate the dispersant, a 5% Ammonia solution (1.4 ml) was added to the mixture solution and stirred for 10 min. The PH-9 was checked for controlled acidity. Ethylene diamine (EDA) solution (0.76 ml) was added as the precipitant. The produced precipitant was washed with DI water and ethyl alcohol after being agitated for a set amount of time. After washing, the precipitant dried at 120 ^oC for 1hr. Then it was calcined at 450 ^oC -600 ^oC for 1hr to get ITO nanopowder.

2.3. Preparation of Electrode

Flexible electrodes of Polyethylene terephthalate (PET), measuring 1x1 cm², were cut into pieces and pre-cleaned using acetone, ethanol, and DI water. Separately, dispersions of ZnO NPs and ZnO NPs/ITO NPs (40 mg each) in 200 μL of DI water were agitated for four hours. The dispersions were then coated onto the pre-cleaned PET electrodes using spin coating and annealed in an oven at 70 °C for 25 minutes. After the annealing process, the electrodes were submerged in an ethanol solution (5 mL) containing 0.5 mM N719 for 12 hours. The platinum (Pt)/PET counter electrode was constructed using the same PET electrode.

2.4. Measurements of Dye Adsorption Levels

In a separate process, the annealed electrodes were submerged in ethanol (5 mL) solutions of N719 (0.5 mM) for 12 hours. The electrodes coated with ZnO NPs and ZnO NPs/ITO NPs were immersed in a 1 M NaOH solution (5 mL) for 12 hours to extract the dye loaded on the electrodes. Any remaining dyes were removed using water. The amounts of dye in the extractants were calculated using calibration curves and the calorimetric method.

2.5. Electrochemical Measurements (I-V)

The PET flexible electrode substrate pre-cleaning process involved the use of acetone, water, and UV light irradiation in a vacuum for 5 minutes. The dispersions of ZnO NPs and ZnO NPs/ITO NPs were separately agitated in 200 μL of water for 4 hours. Using a spin coater at 2000 rpm, the dispersions were coated onto a 1x1 cm2 area of the pre-cleaned PET electrode and dried separately. The ZnO NPs and ZnO NPs/ITO NPs electrodes were then annealed in the oven at 70 °C for 25 minutes. After that, they were immersed in ethanol (5 mL) solutions of N719 (0.5 mM) dyes for 12 hours separately. The ZnO NPs and ZnO NPs/ITO NPs photo-cathode films, with a thickness of 0.144 mm, on the PET electrode were assembled with the platinum (Pt)/PET counter electrode. Redox electrolytes (0.3 M KI, 0.05 M I2, and 10 mL of acetonitrile solvent) were added between the two constructed film electrodes on PET. The I-V measurement was performed using a blue (430 nm) light-emitting diode (LED) light source with a ZAHNER, Xpot,26356 German instrument. The total PCE (Photovoltaic Conversion Efficiency) was calculated using the equation below, based on the intensity of the incident light.

$$\mathit{\eta }=\frac{{\mathbf{J}}_{\mathbf{s}\mathbf{c}}{\mathbf{V}}_{\mathbf{o}\mathbf{c}}}{{\mathbf{P}}_{\mathbf{i}\mathbf{n}}}\mathbf{F}\mathbf{F}$$

(1)

where ${\mathit{P}}_{\mathit{i}\mathit{n}}$ is light incident power, ${\mathit{V}}_{\mathit{o}\mathit{c}}$ is the open-circuit voltage, ${\mathit{J}}_{\mathit{s}\mathit{c}}$ is the circuit current density and FF is the fill factor.

3. Results and Discussions

3.1. Characterizations of Composites

TEM images were used to characterize the size and shape of the created nanocomposites, specifically the nanograins of ZnO NPs and ZnO NPs@ITO NPs. The mean diameters measured for these nanograins were 15.22±11 nm and 14.54±16 nm, respectively, which align with previously published values [30]. These measurements can be found in Figure 1.

However, a ZnO NPs@ITO NPs (10 wt%) indicated the presence of smaller nanograins. The results suggest that the combination of ZnO NPs and ITO NPs of different sizes leads to attractive interactions between them. Evidence of the beneficial properties of these nanoparticles can be seen in TEM Figure 1(a) and (b), where the ZnO NPs have formed hexagonal structures, with sphere-like nanoparticles visible in certain areas. Across all particle categories, a range of dimension sizes can be observed, but the average size for composite ZnO NPs and ITO NPs is approximately 12-16 nm. The calculated sizes using TEM are 15.22±11 nm and 14.54±16 nm, respectively, which suggests the possible formation of a heterojunction between them.

Furthermore, Figure 1(a) and (b) reveal that the incorporation of ITO NPs on top of ZnO NPs appears to increase the surface roughness. Supporting this observation, the size distribution histograms shown in Figure 1(c) and (d) for ZnO NPs and ITO NPs confirm that the majority of the particles fall within the range calculated using TEM. In Figure 1(e) and (f) of ZnO NPs in SEM, the images show a uniform dispersion of hexagon-shaped nanoparticles. The SEM analysis also reveals the homogeneous and smooth surface morphology of the ZnO nanoparticles. In Figure 1(f), when the ZnO NPs are treated with ITO NPs, there is a noticeable change in morphology. This change can be attributed to surface interactions between the two types of nanoparticles. Interactions between ZnO NPs and ITO NPs may result in the adsorption or deposition of ITO NPs onto the surface of ZnO NPs, modifying their surface properties and altering their morphology. These interactions could involve chemical reactions at the nanoparticle surfaces, potentially leading to the formation of new compounds or surface modifications that impact the morphology of ZnO NPs. The specific reasons for these morphological changes depend on experimental conditions, nanoparticle characteristics, and interaction mechanisms between ZnO and ITO NPs in each study mentioned. Further analysis and characterization techniques are necessary to determine the exact mechanisms responsible for the observed changes.

The EDX pattern (Figure 1(g)) confirms the presence of zinc (Zn) and oxygen (O) as the only elements detected in the sample, suggesting that no other trace elements are present in the synthesized nanopowder. The atomic and weight percentages of the components in ZnO NPs reveal that the particles are composed entirely of Zn and O. This finding confirms the atomic ratio of Zn and O shown in Figure 1(g) to be almost equal, indicating that the quantities of these elements involved in the reaction or compound formation of ZnO are as shown. In Figure 1(h), the EDS analysis also shows the elemental components of the collective part to be oxygen (O), zinc (Zn), tin (Sn), and indium (In). This indicates the presence of ZnO and indium tin oxide (ITO). The weight percentage (wt%) and atomic percentage (At%) values of each element in Table 1 support this finding.

These values correspond to the expected elements for Figure 1(h). However, the presence of carbon (C) in Figure 1(h) is unexpected based on the composition in Table 1. The material of ZnO/ITO does not list carbon as an elemental component of the ZnO/ITO material. Therefore, the carbon detected in Figure 1(h) may be attributed to small impurities or contaminants. It is possible that trace amounts of carbon were present in the sample, resulting in its detection during the analysis.

As shown in Figure 2(A) and Table 2(A), the XRD diffraction peak values correspond to the d-spacing, indices, and 2theta angles for ZnO NP samples obtained through the sol-gel synthesis method at different annealing temperatures. The subsequent sections of the table provide the same index information at 2θ = 31.73°C, 34.42°C, 36.26°C, 47.53°C, 56.53°C, 62.87°C, 66.35°C, 67.86°C, 69.04°C, respectively, for the (100), (002), (101), (102), (110), (103), (200), (112), and (201) planes for the ZnO NP obtained at annealing temperatures of 450°C. The same indices are also provided for 300°C, 350°C, 400°C, and 500°C, which is in agreement with the reported scholars [31]. This indicates that pure crystalline ZnO NPs have been prepared. The ideal levels of crystallinity and purity of a single phase of ZnO NPs were found using temperatures ranging from 300 to 500°C. However, at an annealing temperature of 450°C, it reveals almost the same d-spacing values and 2theta values as the standard reported values. When analyzing the diffraction patterns of ZnO NPs, certain characteristic peaks corresponding to specific crystallographic planes within the hexagonal structure of ZnO can be observed. These peaks can be indexed by JCPDS card No. 01-079-2205 [32], allowing researchers to identify and confirm the crystal structure of the ZnO nanoparticles. The cubic-like structure (JCPDS 06–0416) [33] of the ITO NPs XRD peak diffraction at 2θ = 21.77°C, 30.74°C, 35.72°C, 37.90°C, 42.21°C, 46.04°C, 51.35°C, 56.27°C, 59.55°C, and 60.91°C for the planes (211), (222), (400), (411), (332), (431), (440), (433), (611), and (622) has been observed, respectively. It is also observed that the degree of intensity of the ZnO NPs increases as the temperature rises to 450°C. In this case, as the temperature increases, the atoms within the ZnO NPs can rearrange themselves into a more ordered lattice, resulting in increased crystallinity. However, as the temperature continues to rise to 500°C, the intensity of all the diffraction peaks decreases. A decrease in peak intensity suggests a reduction in the scattering of X-rays, which could be attributed to a decrease in the crystalline quality of the ZnO nanoparticles. At higher temperatures, there might be factors such as grain growth, lattice defects, or even phase transformations that can lead to a decrease in the crystalline quality and, consequently, a decrease in peak intensity.

The details provided in Figure 2(A) would show the variation in peak intensities as a function of temperature, visually representing the changes in crystallinity and the decreasing peak intensities.

As can be seen in Figure 2(B) and Table 2(B), the XRD peaks and peak positions of ZnO NPs have changed in line with the addition of ITO NPs. This demonstrates that the structure of ZnO NPs is impacted by the ITO NPs. All the known ITO NPs XRD peaks with their respective induced planes can surely be found in the composite of ZnO NPs/ITO NPs. However, a shift in the peak positions of ZnO NPs has been observed after the addition of ITO NPs. For instance, the peak positions of 31.73 ^oC, 34.42 ^oC, and 36.26 ^oC for ZnO NPs were shifted to 31.70 ^oC, 34.37 ^oC, and 36.29 ^oC, respectively, after the addition of ITO NPs. This indicates that ITO NPs can impact the crystallography of ZnO NPs, which may be suitable for another application. The lattice parameters for ZnO NPs and ZnO NPs@ITO NPs, calculated from XRD peaks, are 3.124 Å and 4.642 Å, respectively, and 3.214 Å and 4.725 Å, respectively.

3.2. Optical Properties

As can be seen in UV-Vis Figure 3 (A) and (B), the highest peaks in the spectra of ZnO NPs are located at 380 nm, regardless of the annealing temperatures that were used. The redshifted wavelength of ZnO NPs, on the other hand, only becomes noticeable at certain temperatures. The actual band gap shifts along with the temperature of the ZnO NPs as it goes through its range of different temperatures. However, the redshift wavelength with the new band spectra of ZnO NPs appeared at 428 nm after a 10 wt% mass of ITO NPs was added to ZnO NPs (seen in Figure 3 (B)). This can be attributed to the electron transition from the valence band (VB) to the conduction band (CB) of the energy level. The influence of ITO NPs on the shift of wavelength from the ultraviolet band of the spectra to the visible band (380 nm - 428 nm) is possible. Although exposure to visible light does not pose any danger to humans. Therefore, the composite of these materials may have several uses in various contexts. Examples include photocatalytic degradation, solar energy, and other similar processes.

The Tauc plots seen in Figure 3 (C), (E), and Table 1 of ZnO NPs and ZnO NPs/ITO NPs demonstrate, the variation of the band gap of ZnO NPs at different annealing temperatures and the band gap of ZnO NPs at different wt % of ITO NPs. Consequently, as temperature raised from 300⁰C-450⁰C the band gap of the shows decreasing, but after the 450⁰C to increase. Indicating the annealing temperature can influence the band gap of the materials which corresponded to the conductivity of the materials. As seen Figure 3(D) and Table 1, the small band gap seen at 450⁰C. In addition, when ZnO NPs treated by different wt% of ITO NPs, the change in band gap of ZnO NPs at 10 wt% of ITO NPs reduced to 2.88eV from 2.94eV (seen Figure 3(E) & (F) and Table 1,). The interaction between ZnO and ITO NPs can lead to chemical reactions or alloying at the interface. This can introduce new energy levels or modify the electronic structure of the ZnO NPs, affecting the band gap. The presence of ITO NPs, which typically have a lower band gap than ZnO, can influence the overall band gap of the nanocomposite. And dopants can create energy levels within the band gap, influencing its width. The nature and concentration of defects or dopants can vary with the annealing temperature or the weight percentage of ITO NPs, leading to changes in the band gap.

3.3. Photoluminescence Properties

During the excitation process, a material absorbs photons of specific energy [9], causing electrons to move from the valence band to the conduction band or to higher energy states within the band gap. This process creates electron holes in the valence band. As a result, when a material emits light after absorbing photons, it is known as photoluminescence. Figure 4 displays the photoluminescence (PL) profiles of ZnO nanoparticles (NPs) at different temperatures: 300, 350, 400, 450, and 500 °C. These PL profiles provide information about the emission of light at specific wavelengths, revealing the presence of different energy levels and defects in the material. For the ZnO NPs, the broad emission band is a result of the superimposition of a major peak and a broad emission, with the peak occurring at approximately 524 nm when annealed at 450 °C. This indicates that the optical characteristics of photoluminescence can be affected by the annealing temperature. As seen in Figure 4, five clear peaks at 498 nm, 506 nm, 510 nm, 515 nm, and 523 nm for 300 ⁰C, 500 ⁰C, 350 ⁰C, 400 ⁰C, and 450 ⁰C ZnO NPs respectively. Different flaws, including oxygen intermediate (O_i), zinc interstitial (Zn_i), oxygen vacancies (V_o), zinc vacancies (V_zn), and oxygen antistites (O_zn), were thought to be the possible causes of the deep-level emission seen in the visible range. Because according to Gaussian fitting [34], it was used to look at the broad spectrum in the visible region and study the blue (470 nm and 492 nm) and green (522 nm) emissions. The blue fluorescence at 498 nm was generated through the recombination of zinc interstitial (Zn_i ) energy level and zinc vacancy (V_Zn). The blue fluorescence peaks at 498nm were reported by Lakshi Saikia et al. to the transfer of electrons from the upper valence band to the zinc interstitial (Zni ) site [35]. Oxygen vacancies, created at the deep donor level in the material’s bandgap, are responsible for the 523 nm green emission peak. Whenever the temperature of the substrate rises, the visible light intensity falls, demonstrating that the substrate temperature plays a significant role in the creation of different defects throughout the lattice of ZnO NPs.

Figure 5 displays the PL spectra obtained from our experiments to examine the impact of ITO (indium tin oxide) nanoparticles on the optical characteristics of ZnO NPs/ITO NPs. We investigated using photoluminescence (PL) spectroscopy, which allows us to study light emissions from the materials under specific conditions. In this study, we recorded the PL spectra of a composite of ZnO NPs and ITO NPs (ITO NPs/ZnO NPs) materials at low temperatures ranging from 84K to 300K. The low-temperature photoluminescence measurements and optical transmittance analysis experiments were carried out at an optimized temperature of 450°C. In Figure 5, the low-temperature photoluminescence characteristics of the ZnO NPs@ITO NPs nanostructures, we observe a single emitting band, which corresponds to a broad visible emission peak centered around 535 nm. This emission is observed within the low-temperature range of 84K to 300K for the ZnO NPs@ITO NPs hybrid nanostructure. In summary, these findings provide valuable insights into the optical behavior of hybrid nanostructures and contribute to our understanding of the interaction between ITO NPs and ZnO NPs.

It is evident that the band edge emission increases in the 84K treated sample compared with 300K. This can be attributed to the lower temperature treatment reducing the impurities in the materials and revealing the semiconductor’s photoluminescence characteristics. On the other hand, the intensity of the broad emission decreases significantly from 84K to 300K. Thus, room temperature can affect the photoluminescence behavior of the materials. However, when the bare ZnO NPs@ITO NPs sample is excited by the laser source and its electrons are stimulated to the conduction band, only a small portion of these electrons return directly to the valence band, while most of them become trapped in the defect levels. As a result, the electron from the conduction band is easily trapped back into the defect states, causing a broad hump in the visible region.

3.4. I-V Performance of F DSSCs

The impact of ITO NPs on FDSSC performance has not been assessed yet, but it effectively produces a quick photocurrent response. As shown in Figure 6 and Table 3, loading the optimized ITO NPs (10 wt%) onto the PEN/Pt substrate enhances the current density from 7.65+0.13 to 11.420±0.14 mA/cm2. As a result, the PCE increases from 2.198±0.14 to 6.680+0.12%. The interaction between ITO NPs and ZnO NPs augments charge separation decreases charge recombination, and boosts charge transport at ZnO NPs. These factors are deemed crucial for enhancing photocurrent production. Table 3 provides data on the I-V performance of FDSSCs with ZnO NP@ITO NP photocathodes at different weight percentages of ITO NPs loaded on ZnO NPs. This data reveals a trend where the photocurrent density (Isc) and efficiency (η%) increase with higher weight percentages of ITO NPs, up to a certain point. This indicates that the incorporation of ITO NPs enhances the performance of the solar cells, but there may be an optimal weight percentage beyond which further loading does not significantly improve performance. Figure 6(A) displays the power conversion efficiency (PCE) of FDSSCs with ZnO NPs at different weight percentages of ITO NPs. It shows that the PCE varies, indicating that the interaction between the surface of ZnO NPs and ITO NPs differs depending on the weight percentage of ITO NPs. This variation in interaction leads to differences in the performance of the FDSSCs, highlighting the importance of optimizing the weight percentage of ITO NPs for maximum efficiency.

Figure 6(B) (a), (b), (c), and (d) demonstrate the I-V parameters at different mass loadings of ITO NPs. It shows that at a ZnO NPs/ITO NPs ratio of 10 wt%, the dye loading performance is higher. This indicates that at this specific weight percentage, there is optimal light absorption and performance, leading to enhanced efficiency. Thus, the findings suggest that the performance of FDSSCs is influenced by the weight percentage of ITO NPs deposited on ZnO NPs. Optimizing this weight percentage is crucial for maximizing efficiency, as it affects the interaction between the nanoparticles and ultimately determines the overall performance of the solar cells. Overall, the results suggest that the incorporation of ITO NPs into FDSSCs leads to significant improvements in their performance, primarily through enhanced charge transport and reduced recombination, ultimately resulting in higher efficiency.

Table 4 presents a comparison of the performance of different flexible electrodes for DSSCs using various materials. The table includes information on the materials, deposition techniques, working electrode (WE), counter electrode (CE), power conversion efficiency (PCE) in %, and related references. The study reported a significant improvement in the performance of FDSSCs when ITO NPs were added to ZnO NPs, with the ZnO NPs/ITO NPs DSSC showing an approximate 6.680±0.12 nearly double improvement.

Furthermore, the combination of ZnO NPs solar cells, N719 dye, and ITO NPs had a synergistic effect, leading to improved performance of the DSSCs. ITO NPs are excellent electron donors and acceptors. This study clearly demonstrates the dual functionality of photo-excited ITO NPs as both electron donors and acceptors. ITO nanoparticles (NPs) are widely known for their remarkable abilities in photo-induced electron transfer and light harvesting, which enhance their photocatalytic and light-energy conversion capabilities. The presence of ITO NPs improves photocurrent production, dye adsorption, light harvesting, PCE efficiency, recombination reduction, and mobility enhancement. Lastly, the use of ITO NPs holds the potential for achieving photogenerated charge separation.

4. Conclusions

In conclusion, the comprehensive analysis of the ZnO NPs and ZnO NPs@ITO NPs nanocomposites reveals significant enhancements in structural, optical, and electronic properties upon the incorporation of ITO. TEM and SEM imaging confirm uniform dispersion and surface morphological changes indicative of potential heterojunction formation. EDX analysis validates the elemental composition, while XRD patterns illustrate increased crystallinity and structural modifications. UV-Vis spectra demonstrate a redshift, suggesting applications in photocatalysis and solar energy. Band gap analysis and PL spectra indicate the influence of ITO on optical properties, reducing the band gap and altering emission behavior. The incorporation of 10 wt% ITO NPs into ZnO NPs notably improves the performance of flexible dye-sensitized solar cells, with substantial increases in current density and power conversion efficiency. These findings highlight the critical role of ITO NPs in enhancing the functional properties of ZnO NPs, paving the way for their application in advanced optoelectronic devices.