Enhancement of Photocatalytic Activity and Microstructural Growth of Cobalt-Substituted Ba 1 − x Co x TiO 3 {x = 0, . . . , 1} Heterostructure

: The photocatalytic degradation process and absorption kinetics of the aqueous solution of the Cibacron Brilliant Yellow 3G-P dye (Y) were investigated under UV-Vis light. Pure barium titanate BaTiO 3 (BT) and cobalt ion-substituted barium Ba 1 − x Co x TiO 3 (x = 0, . . . , 1) nano-compound powders (BCT) were synthesized using the sol–gel method and colloidal solution destabilization, and utilized as photocatalysts. The powder X-ray diffraction (PXRD) crystal structure analysis of the BT nanoparticles (NPs) revealed a prominent reﬂection corresponding to the perovskite structure. However, impurities and secondary phase distributions were qualitatively identiﬁed in the PXRD patterns for x ≥ 0.2 of cobalt substitution rate. Rietveld reﬁnements of the PXRD data showed that the BCT nano-compound series undergoes a transition from perovskite structure to isomorphous ilmenite-type rhombohedral CoTiO 3 (CT) ceramic. The nanoparticles produced displayed robust chemical interactions, according to a Fourier transform infrared spectroscopy (FTIR) analysis. The BT and BCT nanoparticles had secondary hexagonal phases that matched the PXRD results and small aggregated, more spherically shaped particles with sizes ranging from 30 to 114 nm, according to transmission electron microscopy (TEM). Following a thorough evaluation of BCT nano-compounds with (x = 0.6), energy-dispersive X-ray (EDX) compositional elemental analysis revealed random distributions of cobalt ions. Through optical analysis of the photoluminescence spectra (PL), the electronic structure, charge carriers, defects, and energy transfer mechanisms of the compounds were examined. Due to the cobalt ions being present in the BT lattice, the UV-visible absorption spectra of BCT showed a little red-shift in the absorption curves when compared to pure BT samples. The electrical and optical characteristics of materials, such as their photon absorption coefﬁcient, can be gathered from their UV-visible spectra. The photocatalytic reaction is brought about by the electron–hole pairs produced by this absorption. The estimated band gap energies of the examined compounds, which are in the range of 3.79 to 2.89 eV, are intriguing and require more investigation into their potential as UV photocatalysts. These nano-ceramics might be able to handle issues with pollution and impurities, such as the breakdown of organic contaminants and the production of hydrogen from water.


Introduction
The generation of contaminated wastewater during manufacturing and industrial processes [1] poses a significant threat to natural waterways and the purity of finite aquifers [2]. Many industrial waste products [3,4] also contain toxic substances that pollute the environment and exacerbate existing health problems [5]. The textile industry contributes to substantial environmental problems due to the effluent flows that contain dyes [6]. Reactive dyes, such Cibacron Brilliant Yellow 3G-P (Y), are widely used in dyestuffs due to their useful qualities, such as bright colors, water-fastness, and less energy usage during

Experimental Process
A novel sol-gel-assisted solid-phase method for synthesizing nano BT ceramics at high temperatures is described in [61]. The authors demonstrate how the synthesis process affects the performance of the photocatalytic process and the conversion of the tetragonal phase in this study [61]. For that, a typical experiment entailed mixing barium nitrate and cobalt (II) chloride hexahydrate in 60 mL of deionized water with magnetic stirring in the appropriate weighted proportions based on the molar ratio of Ba/Co. In addition, a molar proportion of TiO 2 was dissolved in pure nitric acid while being vigorously stirred using a thermo-magnetic stirrer at 50 • C for two hours to achieve total dispersion and the formation of the intermediate agent [Ti(NO 3 ) 4 ].
The solution containing barium nitrate, cobalt chloride hexahydrate, and dispersed TiO 2 in nitric acid was further treated with 5 mL of ethylene glycol anhydrous to prevent particle agglomeration and facilitate dispersion. The resulting mixture was then stirred at 50 • C for 4 h to form a colloidal gel, which was dried at 100 • C for 12 h. The dried gel was then heated at a rate of 5 • C/min to 1000 • C for 3 h in a muffle oven. The particle size homogeneity of the BCT compound was verified prior to sample removal by allowing the reaction mixture to air-cool to room temperature. Figure S1 shows a flow diagram of the various steps involved in the sample preparation process.

PXRD Analysis
The crystal structure and the phase purity of all samples were determined by powder Xray diffraction (PXRD) analysis. PXRD patterns were obtained using a Bruker D8 Advance instrument with Cu-Kα radiation and a step interval of 0.02 degrees.
The Diffrac Plus software was utilized to identify the material-phase based on the PXRD measurements. Rietveld refinement was used to quantitatively analyze the structural characteristics from the PXRD patterns using the PROFEX BGMN refinement program [62].

TEM Scanning and Energy-Dispersive X-ray Spectroscopy (EDX)
Transmission electron microscopy (TEM) using a FET Tecnai G2 operating at 200 kV revealed the nanostructure and morphology of powdered materials. TEM specimens were prepared by breaking the samples while submerging them in ethanol. A drop of the suspension was then deposited onto a copper grid-supported holey carbon film. Local chemical analysis was performed using an energy-dispersive X-ray spectroscopy (EDX) system coupled with a Carl Zeiss Ultra 55 field-emission scanning electron microscope.

Fourier Transform Infrared Spectroscopy (FTIR)
The Fourier transform infrared spectra (FT-IR) were measured using a Bruker VER-TEX 80V spectrometer, which was configured in the spectral range of 4000 to 400 cm −1 ChemEngineering 2023, 7, 43 4 of 23 (corresponding to terahertz frequencies of 1016 Hz to ultraviolet frequencies of 1012 Hz) at a temperature of 25 • C. The optical resolution of the instrument was <0.06 cm −1 .

Photoluminescence Spectroscopy (PL)
To investigate the optical properties of semiconductors, PL spectra were measured over a spectral range of 300 to 500 nm using two different excitation wavelengths. The measurements were conducted by varying the temperature of the sample between 10 and 450 Kelvin, using a closed-circuit helium cryostat, and two excitation lasers with wavelengths of 266 nm and 447 nm. The RF-5301 PC spectrophotometer equipped with a 290 nm filter was used for the measurements.

UV-Visible Spectroscopy
The UV-visible diffuse reflectance and absorbance spectra of all samples were recorded using a Shimadzu UV-2600 spectrophotometer in the spectral range from 200 to 400 nm.

Photocatalytic Application
Metal/halide-perovskites have gained interest for their potential as photocatalysts due to their adjustable preparation and the ability to alter their bandgap by modulating the ratio of halides and metals. These compounds are intriguing options for photocatalytic applications, according to Schanze Kirk et al. [63]. The photocatalytic activity of the produce BCT samples was evaluated in this study by degrading 10 ppm of Cibacron Brilliant Yellow 3G-P (Y) solution in a cylindrical quartz glass reactor with an effective vessel volume of 80 mL.
Cibacron Brilliant Yellow 3G-P(C 25 H 15 Cl 3 N 9 Na 3 O 10 S 3 ) was obtained from Sigma-Aldrich, a division of Merck KGaA, Darmstadt, Germany. The molecule has three sulfonate groups ( Figure S2), which are negatively charged in aqueous solution. It has a molecular weight of 831.02 g mol −1 , a color index number of 18,972, and a maximum absorption wavelength of 404 nm [64]. Double distilled water was used for all experiments, and nitric acid (purchased from TEDIA, supplier of high-purity solvents and acids, located in Fairfield, USA) and sodium hydroxide (Sigma-Aldrich, a division of Merck KGaA, Darmstadt, Germany) were used to adjust the pH to 5. The dye was used without further purification, and all other chemicals used were of analytical grade unless otherwise stated [65].
The experimental setup involved a 230 V~50-60 Hz, 2066 W UV lamp with a cooling water circuit, which served as a side light source, emitting light at wavelengths of 365 nm and 254 nm. The distance between the photoreactor and the UV lamp was 6.0 cm. A suspension of BCT photocatalysts (at a concentration of 66 ppm) in 50 mL of solution (denoted as Y) was stirred in the dark for 30 min to achieve adsorption-desorption equilibrium before the photocatalytic reaction. After that, the suspension was continuously exposed to UV radiation for 180 min at 25 • C while being aerated with air flowing via a mini-pump at a flow rate of 4.2 L/min. At various time intervals, a sample of the suspension was taken out and centrifuged for 10 min to obtain clear solution of (Y), which was then analyzed for its concentration using a Shimadzu UV-2600 spectrophotometer at 254 nm. The residual rate of (Y) can be calculated using a specific equation [66]: where A 0 is the initial concentration of (Y), A t is the concentration of (Y) after reacting t minutes. Table 1 (below) provides an overview of multiple researches investigating the use of photocatalysts to remove different organic pollutants, with a specific focus on the BT catalyst. Table 2 organizes and presents these research findings.

Qualitative PXRD Analysis
Good crystallinity is an essential property of nanoparticles as it influences their stability, reactivity, and overall performance in a variety of applications. The pure BT nanoparticle powder, in this case, appears to have a high crystallinity degree, which could make it suitable for a variety of applications, according to the results of the PXRD study. Figure S3 displays the PXRD pattern of the BT nanoparticle powder as it was formed. The PXRD data displays distinctive reflections, demonstrating that the particles have an extremely ordered atomic structure. The findings suggest that BT nanoparticles crystallize exclusively in the perovskite phase without passing through any further phases. According to JCPDS files, the appropriate planes for indexing reflections are (hkl). The primary peaks in the PXRD pattern located at 2θ  [81]. Table 3 also shows that the PXRD data of the BCT ceramics exhibit a transitional structure for (x ≥ 0.3). This indicates that the perovskite structure of BT nanoparticles was maintained and that Co 2+ ions were typically absorbed into the lattice for low bulk density (x = 0.3). Furthermore, it shows that adding more Co ions to BT might possibly replace Ba, raising the 45.21 • characteristic peak to lower 2θ • values, and that no secondary phases result from Co substitution in the BT lattice in this domain. Carrying on this study of phase's identification, a scan match was performed via comparison with standard JCPDS PDF data base structures files reported in the literature that indicate the presence of intermediary phases for the formation of x ≥ 0.3, as labeled in Figure 1. The average particle size was calculated using the classical Scherer formula [87]: In the Sherrer formula, "d" represents the average crystallite size, "k" is the shape factor equal to 0.9, "λ" is the wavelength of the X-rays used (λ = 1.5406 Å), "β" is the FWHM of the characteristic peak, and "θ" is Bragg's diffraction angle. This formula only considers the influence of crystallite size on the PXRD peak broadening. The results presented in Table 3 indicate that all of the obtained crystallite sizes fall within the range of 56-114 nm, suggesting that an increase in cobalt concentration is accompanied by a decrease in particle size. Additionally, a series of phase transitions are exhibited by the Ba-TiO3-CoTiO3 system as the Ba substitution level is increased.   Nevertheless, the system maintains the perovskite structure of BaTiO 3 at a small amount of Ba substitution. As the level of Ba substitution is increased, the crystal structure transforms into the CoTiO 3 ilmenite structure. In the BaTiO 3 -CoTiO 3 system, the phenomena of intermediate phases emerging during the phase transition from perovskite BaTiO 3 to ilmenite CoTiO 3 is well-known. The crystal structure of the material changes from perovskite to ilmenite as the Ba substitution level rises [82][83][84][85]. However, this change does not occur instantaneously. In fact, this transition must occur through the emergence of intermediary phases in which perovskite and ilmenite coexist [86].
An inability to accomplish a direct transformation between the two crystal forms results in the creation of intermediate phases. Since BaTiO 3 and CoTiO 3 have differing lattice properties and crystal symmetries, switching between these two crystal forms causes a substantial alteration in the material's atomic composition. The challenging nature of this transformation leads to the emergence of intermediary phases. The creation of intermediate phases is a natural byproduct of the gradual change from the perovskite to the ilmenite structure. The composition and characteristics of these intermediary phases can change depending on the synthesis conditions, such as temperature, pressure, and annealing time.
As a result, the presence of these intermediary phases, which are expected to be part of the phase transition process, is responsible for the impurities emerging in the samples at higher Ba levels of substitution. It is significant to consider that the development of intermediate phases in the BaTiO 3 -CoTiO 3 system results from the complicated nature of the phase transition between the perovskite and ilmenite structures, not necessarily from poor sample quality.
The average particle size was calculated using the classical Scherer formula [87]: In the Sherrer formula, "d" represents the average crystallite size, "k" is the shape factor equal to 0.9, "λ" is the wavelength of the X-rays used (λ = 1.5406 Å), "β" is the FWHM of the characteristic peak, and "θ" is Bragg's diffraction angle. This formula only considers the influence of crystallite size on the PXRD peak broadening. The results presented in Table 3 indicate that all of the obtained crystallite sizes fall within the range of 56-114 nm, suggesting that an increase in cobalt concentration is accompanied by a decrease in particle size. Additionally, a series of phase transitions are exhibited by the BaTiO 3 -CoTiO 3 system as the Ba substitution level is increased.
With a rise in Co concentration in the solid solution, the unit cell of BCT samples tends to decrease. Examining the cobalt ions in the BCT unit cell could provide insight into this phenomenon. In our case, Co ions with a coordination number of 12 are situated in the A sub-lattice, occupying the Ba site. According to [88], the difference in ion radii between Ba and Co ions refers to the saturation and phase transition processes.

Quantitative PXRD Analysis
The BCT sample underwent Rietveld refinement using PROFEX BGMN software to perform quantitative PXRD analysis. Figures 2 and S4a-j show the BCT's refined PXRD data. The refinement supports the PXRD data analysis findings and confirms the transition from a tetragonal single phase to a rhombohedral phase for all increasing Co specimens. This transition was observed through Rietveld PXRD fitting profiles, as reported by Wang et al. [89], which revealed a typical tetragonal structure with P4mm (99) space group. Table 4 lists the different structural characteristics identified through the refinement of the BCT PXRD data.
perform quantitative PXRD analysis. Figures 2 and S4a-j show the BCT's refined PXRD data. The refinement supports the PXRD data analysis findings and confirms the transition from a tetragonal single phase to a rhombohedral phase for all increasing Co specimens. This transition was observed through Rietveld PXRD fitting profiles, as reported by Wang et al. [89], which revealed a typical tetragonal structure with P4mm (99) space group. Table 4 lists the different structural characteristics identified through the refinement of the BCT PXRD data. Bragg reflections and variations between the experimentally measured patterns and predicted patterns of selected samples were obtained at room temperature. The samples were identified as being single-phase crystalline and chemically pure based on the findings of the Rietveld investigation of PXRD. The structures of all samples were carefully refined, and the results are quite interesting. The unsubstituted and low-substituted samples, limited by x = 0.3, exhibited a single crystal phase, and Rietveld refinement resulted in a tetragonal structure with P4mm space group. The highest substitution sample (x = 1) crystallized in a rhombohedral phase with R-3 space group, as a result of an increasing Co substitution rate, which caused a structural phase transition. For pure BT, the goodness of fit (GOF) was found to be approximately 1.25, while the BCT sample series exhibited a reasonably good fit.   Bragg reflections and variations between the experimentally measured patterns and predicted patterns of selected samples were obtained at room temperature. The samples were identified as being single-phase crystalline and chemically pure based on the findings of the Rietveld investigation of PXRD. The structures of all samples were carefully refined, and the results are quite interesting. The unsubstituted and low-substituted samples, limited by x = 0.3, exhibited a single crystal phase, and Rietveld refinement resulted in a tetragonal structure with P4mm space group. The highest substitution sample (x = 1) crystallized in a rhombohedral phase with R-3 space group, as a result of an increasing Co substitution rate, which caused a structural phase transition. For pure BT, the goodness of fit (GOF) was found to be approximately 1.25, while the BCT sample series exhibited a reasonably good fit.
The effect of Co 2+ content on the lattice parameters (a, c) was estimated from fitting PXRD data, as well as the decrease in tetragonality (c/a) with increasing Co 2+ ratio. The variations in the lattice parameters are due to the incorporation of Co 2+ /Ba 2+ into the lattice. Taking the ionic radius into account, it is believed that Co 2+ (with a radius between 0.58 and 0.90 Å) has a relatively small ionic radius compared to Ba 2+ (with a radius of 1.35 Å). This difference induces a lattice strain, according to Mahmoud et al. [90], and significantly causes the shrinkage of the optical bandgap, as manifested by absorption red shifting in the UV spectra.

FT-IR
The FT-IR spectra of BCT and pure BT are shown in Figure 3.  (Table 5) [91]. Therefore, the obtained results are in good agreement with those of the X-ray diffraction analysis.
Engineering 2023, 7, x FOR PEER REVIEW 10 of Figure 3. FTIR spectra of Ba/Co-substituted barium titanate samples.    Figure 4a reports the surface structure and chemical composition of the Ba 0.4 Co 0.6 TiO 3 sample (x = 0.6) at the nanoscale. This obviously quasi-hexagonal shape is attributable to the phase transition to the R-3 space group. Additionally, the sample's microstructure and grain arrangement are successfully represented. Other samples with a particular x value, selected using a common method, highlight observed phase transitions and are shown in supplementary Figure S5. Indeed: • Figure S5a,b show TEM images for pure BT powder, which were composed of irregular cubic-shaped solids with interplanar spacing d hkl equal to 0.32 nm and a size range between 30 and 114 nm, appearing as several micron-sized solids. Additionally, the highly crystalline surface textures and lack of agglomeration, along with the grain's tendency to grow uniformly, are visible. • Figure S5c,d depicts TEM images of the Ba 0.8 Co 0.2 TiO 3 nano-compound, which had clearly defined quasi-cubic forms, sharp grain boundaries, and little agglomeration. The CoTiO 3 single phase (full cobalt substitution rate) TEM images in Figure S5i,l have the fewest spherical-shaped agglomerations. The average particle size of the CT nanoparticles ranged from 36 to 93 nm, with a constrained size distribution.
These results validate the PXRD studies and demonstrate the existence of a tetragonal phase transition up to x = 0.3 value. Furthermore, TEM images of the BCT complex series reveal that cobalt substitution in the BT lattice has a major impact on the grain size and shape of the samples. However, this effect diminishes with the increasing cobalt ratio in the nanopowder.
It is important to note that the samples' composition was confirmed, and the microstructure and grain arrangement were also considered. To test the composition and elemental integrity of the pure BT and Ba 0.4 Co 0.6 TiO 3 sample we used energy dispersive analysis of X-rays (EDX)-the most trustworthy method. The energy dispersive spectra (EDX) of the BT and BCT for x = 0.6 are shown in Figure 4b,c, respectively. Figure 4b shows that every element is present in the sample, and no necessary element has been left out. No extraneous spectral component is also discernible. The composition and concentration of the components also affect the intensity strength of the visible peaks. structure and grain arrangement were also considered. To test the composition and elemental integrity of the pure BT and Ba0.4Co0.6TiO3 sample we used energy dispersive analysis of X-rays (EDX)-the most trustworthy method. The energy dispersive spectra (EDX) of the BT and BCT for x = 0.6 are shown in Figure 4b,c, respectively. Figure 4b shows that every element is present in the sample, and no necessary element has been left out. No extraneous spectral component is also discernible. The composition and concentration of the components also affect the intensity strength of the visible peaks.  By using elemental energy dispersive spectroscopy, the distribution of the barium, cobalt, and oxygen elements was appropriately described. The EDX findings also showed the presence of titanium, proving that BT nanoparticles were successfully formed and disclosing the substituted and host components of the samples. As a result, the purity and stoichiometry of BT can be deduced, as well as the spectra for BCT compounds (Figure 4c) with x = 0.6, representing the distribution of the various elements present in the spectroscopic localization space in this sample. The absence of a signal for Ti in the BCT (x = 0.6) sample could be attributed to several purposes, such as the amount of Ti present, its position within the surface's heterogeneous distribution, or EDX equipment limitations. For such, there is quantitative information in Table 6 (below) that displays the atomic/weight percentage for various elements. According to TEM data that are roughly identical to those from XRD, the BCT series was able to grow utilizing the sol-gel method.  By using elemental energy dispersive spectroscopy, the distribution of the barium, cobalt, and oxygen elements was appropriately described. The EDX findings also showed the presence of titanium, proving that BT nanoparticles were successfully formed and disclosing the substituted and host components of the samples. As a result, the purity and stoichiometry of BT can be deduced, as well as the spectra for BCT compounds (Figure 4c) with x = 0.6, representing the distribution of the various elements present in the spectroscopic localization space in this sample. The absence of a signal for Ti in the BCT (x = 0.6) sample could be attributed to several purposes, such as the amount of Ti present, its position within the surface's heterogeneous distribution, or EDX equipment limitations. For such, there is quantitative information in Table 6 (below) that displays the atomic/weight percentage for various elements. According to TEM data that are roughly identical to those from XRD, the BCT series was able to grow utilizing the sol-gel method.

UV-Visible
After confirming the acquired structure and phase developed in the selected studies, the required characteristics were analyzed. Optical features of the synthesized complexes are summarized in Figure 5. Figure 5a shows the UV-visible absorption spectra of Ba 1−x Co x TiO 3 samples in the wavelength range of 200-400 nm. The absorption curves of BCT exhibit a red-shift compared to those of pure BT, which is attributed to the significant absorption band of cobalt ions in the 200-250 nm range. These spectral characteristics quantitatively demonstrate that increasing the cobalt content results in increased optical absorption in a manner that is consistent with the findings of Kutapan et al. [92], with a distinct wide band of absorption edge observed in the wavelength range between 270 and 300 nm. To determine the optical bandgap, which is a crucial factor in evaluating the performance of electronic devices, we used the Kubelka-Munk function with the Tauc Plot To determine the optical bandgap, which is a crucial factor in evaluating the performance of electronic devices, we used the Kubelka-Munk function with the Tauc Plot method [93,94] to convert the diffuse reflectance spectra (DRS) into the absorbance coefficient. The Kubelka-Munk [F(R)hν] n function was used to generate a graph, with the y-axis representing the function value and the x-axis representing the energy (E = hν) of the absorbed light. To measure the allowed bandgap directly, the power "n" is set to 2.
To estimate the bandgap, the extrapolated line is used to intersect the plot's energy axis. The curve is extrapolated at the point where it displays a sharp edge. This intercept represents the value of the energy bandgap for the sample. For the Ba 1−x Co x TiO 3 (x = 0.6) sample, we found the intercept value to be 3 eV, as shown in Figure 6a. The bandgap values of all samples {x = 0, . . . , 1}, estimated with the same method ( Figure S6) and presented in Table 7, were consistent with previous reports demonstrating the decrease in the direct band gap value as a function of the cobalt substation rate (Figure 6b). It is worth noting that the bandgap value can decrease to E G = 2.95 [95] due to several factors, including the merging of parent and impurity bands, electronic interactions, scattering by impurities, and lattice compression. These factors contribute to the shrinking of the optical bandgap value, leading to a lesser forbidden band, which is in line with our previous structural studies.
ChemEngineering 2023, 7, x FOR PEER REVIEW method [93,94] to convert the diffuse reflectance spectra (DRS) into the absorba cient. The Kubelka-Munk [F(R)hν] n function was used to generate a graph, w axis representing the function value and the x-axis representing the energy (E = absorbed light. To measure the allowed bandgap directly, the power "n" is set To estimate the bandgap, the extrapolated line is used to intersect the pl axis. The curve is extrapolated at the point where it displays a sharp edge. Th represents the value of the energy bandgap for the sample. For the Ba1−xCoxTi sample, we found the intercept value to be 3 eV, as shown in Figure 6a. Th values of all samples {x = 0, ..., 1}, estimated with the same method (Figure S sented in Table 7, were consistent with previous reports demonstrating the d the direct band gap value as a function of the cobalt substation rate (Figure 6b). noting that the bandgap value can decrease to EG = 2.95 [95] due to several facto ing the merging of parent and impurity bands, electronic interactions, scatter purities, and lattice compression. These factors contribute to the shrinking of bandgap value, leading to a lesser forbidden band, which is in line with ou structural studies.
(a)  Over a temperature range of 10 to 450 Kelvin, the samples were examined usi fluorescence spectrometer. Two excitation sources, with wavelengths of 266 nm a nm, were used to excite the samples. The characterization and improvement of m for photocatalytic applications can benefit from information obtained from photolu cence spectroscopy. The bandgap of the material can be determined by looking at t

PL
Over a temperature range of 10 to 450 Kelvin, the samples were examined using a He fluorescence spectrometer. Two excitation sources, with wavelengths of 266 nm and 447 nm, were used to excite the samples. The characterization and improvement of materials for photocatalytic applications can benefit from information obtained from photoluminescence spectroscopy. The bandgap of the material can be determined by looking at the peak position in the photoluminescence spectrum, which is crucial for finding out its electrical structure and optical characteristics.
The analysis of the emission at the violet region between 400 and 450 nm is shown in Table 8. For all curves of Ba 1−x Co x TiO 3 , {x = 0, . . . , 0.4}, the emission was observed to be sharp, and the cobalt-barium substitution resulted in a reduction in the emission intensity. Figure 5b illustrates how point defects, such as vacancies and complexes with barium interstitials, affect the visible emission. For samples with x values ranging from 0.5 to 1, the emission spectra were examined as well at a second excitation wavelength of 340 nm. This excitation wavelength corresponds to a defect emission that can occur via several different routes involving a variety of states inside the allowed band gap. This suggests that PL and the localized states within the band gap are tightly connected. With an excitation wavelength of 447 nm and an emission peak centered around 340 nm, the sample with x = 0.6 showed both emission peaks at 340 nm and 430 nm. This implies that both values are lower than the band gaps for these samples according to the findings observable in [96]. Understanding a material's photocatalytic performance requires knowledge about the creation and recombination of charge carriers, which photoluminescence can provide. It is widely recognized that the probability of electrical transitions between the valence and conduction bands, which lead to PL emission, is increased by the presence of localized states within the band gap. The violet emission detected in the Ba 1−x Co x TiO 3 samples is attributed to surface-localized states and a photogenerated hole recombining with a single ionized charged state. The PL emission intensity is greatly influenced by the interaction between the sample and the excitation wavelength. Adding more cobalt seemingly reduces the luminescence of the 430 nm peak, which is connected to the disappearance of barium anion vacancies. Prior research [97] has shown that PL emission in semiconductors occurs via a variety of paths involving a variety of states inside the forbidden band gap. PL emission is intimately tied to localized states within the band gap. In the case of Ba 1−x Co x TiO 3 samples, the valence band is made up of oxygen 2p states, while the conduction band is made up of barium s, titanium s, and d states. The band gap may become populated with delocalized electronic states as a result of electron transport between the barium and titanium ions. The production of clusters (such as TiO 2 or TiO 5 ) in samples with x values of 0.5 to 1 is thought to be responsible for the occurrence of s and p states inside the band gap energy.

Photocatalytic Application
Experiments were carried out to compare the activities of different Ba (1−x) Co (x) TiO 3 photocatalysts on the decolorization rate. Cibacron Brilliant Yellow 3G-P dye cannot be broken down without catalysts when exposed to UV-Vis light. The amount of color removed was estimated by taking absorbance measurements at 365 nm. Figure 7a presents correlating results comparing the photocatalytic degradation of CBY 3G-P utilizing the photocatalysts Ba 1−x Co x TiO 3 under 180 min of irradiation. The absorbance maxima of this dye appear to occur at wavelengths of 267 nm, 292 nm, and 400 nm. The decolorization of the dye solution with Ba 1−x Co x TiO 3 catalysts is shown in Figure S7, with kinetic studies every 20 min demonstrated slower photocatalytic reaction rates. This work was repeated for all samples to compare the photocatalytic degradation rates. The sample solutions' starting pH was 5. According to the obtained data, the photocatalytic activity of the Ba1−xCoxTiO3 samples increases as the cobalt concentration rises from x = 0 to x = 0.6. This observation could be explained by the presence of more active sites on the surface of the photocatalysts and the subsequent production of more radicals, such as (-OH).
Typically, in most instances, conduction band (CB) electrons produced by photoexcitation are moved to adsorbed oxygens to create superoxide radical anions (O2•−), while the valence Band (VB) holes oxidize adsorbed water molecules to generate •OH radicals that participate in the degradation of dyes. Furthermore, VB holes created in the semiconductors can also oxidize adsorbed dye molecules into CO2 and H2O. However, the actual photocatalytic degradation mechanism can be comprehended based on the relative positioning of the semiconductor VB and CB potentials in relation to •OH/H2O, O2/O2•−, and the HOMO-LUMO levels of the molecule being degraded. To illustrate the photocatalytic mechanism, energy level diagrams (ELD) are created by calculating the relative band edge positions of the photocatalysts using empirical formulas [100].
Calculated results are summarized in Table 9 (below) with:   With 10 ppm of Ba 0.4 Co 0.6 TiO 3 photocatalysts, the reaction completed at a pH of 4.5 resulted in a 84.61% degradation rate ( Figure S7). By checking the PXRD attributed pattern (x = 0.6), we can observe the coexistence of secondary phase BaCo 9 O 14 that generally does not exhibit significant catalytic activity. As observable in similar studies [98,99], this molecule is a magnetic material at room temperature, with interesting electronic transport properties. BaCo 9 O 14 is often used as a reference material to study the magnetic and transport properties of cobalt and oxygen-based materials. The conclusion gathered from this implies that, for the situation of x = 0.6 cobalt substitution rate, this phase does not have a photocatalytic effect on the catalyst, which characterizes the primary phase of composition. The catalyst's dye breakdown rate is significantly accelerated by increasing the cobalt content. This finding suggests that, during photochemical conversion, Co 2+ is produced from Co 3+ , providing additional Co 2+ to interact with H 2 O 2 during dye degradation (Equation (3)): It should be noted that the results presented in this study are consistent with those of a previous study [100]. The results also indicate that the Ba 1−x Co x TiO 3 heterostructure has a similar effect on the dye breakdown process (as shown in Figure 7a). For values of x ranging from 0.1 to 0.9, the Ba 1−x Co x TiO 3 photocatalysts progressively enhanced the decolorization rate of Cibacron Brilliant Yellow 3G-P dye over a period of 180 min, resulting in degradation efficiencies of 32.93%, 49 As a result, it was revealed that Cibacron Brilliant Yellow 3G-P pollutant degradation efficiency has increased. A drop in degradation efficiency was seen as the catalyst concentration was increased further. This occurs because, once the concentration of photocatalysts rises beyond a certain limit, the solution becomes disordered and UV radiation screens out the reaction, reducing the degradation efficiency. The photocatalytic activity of x = 0.6 showed the maximum degradation efficiency of 84.61% (Figure 7b).
According to the obtained data, the photocatalytic activity of the Ba 1−x Co x TiO 3 samples increases as the cobalt concentration rises from x = 0 to x = 0.6. This observation could be explained by the presence of more active sites on the surface of the photocatalysts and the subsequent production of more radicals, such as (−OH).
Typically, in most instances, conduction band (CB) electrons produced by photoexcitation are moved to adsorbed oxygens to create superoxide radical anions (O 2 •−), while the valence Band (VB) holes oxidize adsorbed water molecules to generate •OH radicals that participate in the degradation of dyes. Furthermore, VB holes created in the semiconductors can also oxidize adsorbed dye molecules into CO 2 and H 2 O. However, the actual photocatalytic degradation mechanism can be comprehended based on the relative positioning of the semiconductor VB and CB potentials in relation to •OH/H 2 O, O 2 /O 2 •−, and the HOMO-LUMO levels of the molecule being degraded. To illustrate the photocatalytic mechanism, energy level diagrams (ELD) are created by calculating the relative band edge positions of the photocatalysts using empirical formulas [100].
Calculated results are summarized in Table 9 (below) with:  Table 9. Calculated values of valence and conduction band positions of Ba 1−x Co x TiO 3 (x = 0, . . . , 1). The energy level diagram (ELD) presented in Figure 8 provides insights into the mechanism of photocatalytic degradation for the sample with a substitution rate of x = 0.6 cobalt, and Supplementary Figure S8 shows ELDs for the rest of the studied samples. The potentials shown in the ELDs are referenced to normal hydrogen electrode (NHE) potentials. From Figure 8, it can be observed that E CB = −0.455 eV is higher than the (O 2 •−) formation potential of +0.13 eV, which leads to a reduction in the dissolved oxygen required to produce O2•− radicals. ChemEngineering 2023, 7, x FOR PEER REVIEW 20 of 26 Figure 8. Schematic ELD of Ba0.4Co0.6TiO3 with respect to potential for the generation of (O2•−) (E°(OH/H2O)) and O2•− (EO2/ O2•−) radicals.

Conclusions
An investigation of the phase transition, demonstrated by the BaTiO3-CoTiO3 system when the Ba substitution level is increased, and the optical properties in the entire margin of cobalt substitution on the BaTiO3 A-site was performed to enhance the photocatalytic activity. Successful synthesis of the BCT Cobalt ion-substituted barium Ba1−xCoxTiO3 (x = 0 ... 1) nanostructure powders was accomplished by destabilizing colloidal solutions. This substitution was assessed using a number of different techniques. A structural analysis was performed using TEM micrographs and confirmed the presence of pseudo-cubic phases ranging in size from 30-114 nm, which is attributable to the tetragonal phase of BCT. This phase is also predominant in the PXRD patterns for x = 0, 0.1, 0.2, and 0.3, indicating high crystallinity in the perovskite structure. As the cobalt concentration increases to x = 0.3, the transition to the isomorphous ilmenite-type rhombohedral CT ceramic phase is observed, accompanied by the appearance of secondary phases. The Rietveld approach, with an intriguing profile fit that produced lower reliability factors, confirms this logical transition. The unit cell characteristics were reduced by raising the cobalt amount in the BCT nano-compounds series, confirming this effect. The elemental energy dispersive

Conclusions
An investigation of the phase transition, demonstrated by the BaTiO 3 -CoTiO 3 system when the Ba substitution level is increased, and the optical properties in the entire margin of cobalt substitution on the BaTiO 3 A-site was performed to enhance the photocatalytic activity. Successful synthesis of the BCT Cobalt ion-substituted barium Ba 1−x Co x TiO 3 (x = 0 . . . 1) nanostructure powders was accomplished by destabilizing colloidal solutions. This substitution was assessed using a number of different techniques. A structural analysis was performed using TEM micrographs and confirmed the presence of pseudo-cubic phases ranging in size from 30-114 nm, which is attributable to the tetragonal phase of BCT. This phase is also predominant in the PXRD patterns for x = 0, 0.1, 0.2, and 0.3, indicating high crystallinity in the perovskite structure. As the cobalt concentration increases to x = 0.3, the transition to the isomorphous ilmenite-type rhombohedral CT ceramic phase is observed, accompanied by the appearance of secondary phases. The Rietveld approach, with an intriguing profile fit that produced lower reliability factors, confirms this logical transition. The unit cell characteristics were reduced by raising the cobalt amount in the BCT nano-compounds series, confirming this effect. The elemental energy dispersive spectroscopy (EDX) of the x = 0.6 confirmed sample, validated the accomplishment of growth, and demonstrated random distributions of cobalt ions. The formed nanoparticles were found to have strong chemical interactions, as revealed by Fourier transform infrared spectroscopy analysis.
Optical tests were performed on the samples to investigate the effects of the A-site replacement rate, and a small red-shift was observed in the absorption curves of BCT compared to pure BT, as detected by PL and UV-visible absorption spectra. The band gap energy of BCT decreased as the barium ion concentration decreased, from 3.7 to 2.8 eV, which enhanced the photocatalytic activity. With a maximum photo-degradation of 84.61% found for x = 0.6, the investigation showed that increasing the quantity of cobalt in the BCT nanoparticles improved the photocatalytic efficiency. As a result, it may be concluded that the catalyst has the potential to selectively degrade dyes in water through photocatalysis.
Supplementary Materials: The following supporting information can be downloaded at: https: //www.mdpi.com/article/10.3390/chemengineering7030043/s1, Figure S1: Flow chart of the sol-gel processing of (x = {0, . . . , 1}) powder ceramics. Figure S2: Characteristics and chemical formula of Cibacron Brilliant Yellow 3G-P (Y). Figure S3: Powder X-ray diffraction pattern of synthesized pure BT nanoparticles heated at 1000 • C. Figure   Funding: This research received no specific grant from any funding agency in the public, commercial, or not-for-profit sectors.

Data Availability Statement:
The generated and analyzed data during the current study are included within the article and can be obtained from the corresponding authors upon reasonable request.

Acknowledgments:
The results presented are a part of the Ph.D. thesis of Sana Jebali (SJ), realized at LR19ES20: Resources, Materials and Ecosystems (RME), Faculty of Sciences of Bizerte, supervised by Walid Oueslati (WO). SJ acknowledges WO for the original idea of the work, the fruitful discussions about perovskite materials (synthesize and properties), her main contribution, respectively, in the acquisition of experimental results, draft paper writing and the proof reading of the final manuscript.

Conflicts of Interest:
The authors declare no conflict of interest.