Understanding the Role of Silver Nanostructures and Graphene Oxide Applied as Surface Modification of TiO2 in Photocatalytic Transformations of Rhodamine B under UV and Vis Irradiation

This work is focused on photocatalytic properties of titanium dioxide thin coatings modified with silver nanostructures (AgNSs) and graphene oxide (GO) sheets which were analyzed in processes of chemical transformations of rhodamine B (RhB) under ultraviolet (UV) or visible light (Vis) irradiation, respectively. UV-Vis spectroscopy was applied to analyze the changes in the RhB spectrum during photocatalytic processes, revealing decolorization of RhB solution under UV irradiation while the same process coexisting with the transformation of RhB to rhodamine 110 was observed under Vis irradiation. The novelty of this study is the elaboration of a methodology for determining the parameters characterizing the processes occurring under the Vis irradiation, which enables the comparison of photocatalysts’ activity. For the first time, the method for quantification of rhodamine B transformation into rhodamine 110 in the presence of a semiconductor under visible light irradiation was proposed. Photocatalysts with various surface architectures were designed. TiO2 thin coatings were obtained by the sol-gel method. GO sheets were deposited on their surface using the dip-coating method. AgNSs were photogenerated on TiO2 or grown spontaneously on GO flakes. For characterization of obtained photocatalysts, scanning electron microscopy (SEM), X-ray diffraction (XRD) and diffuse-reflectance spectroscopy (DRS) techniques were applied. The results indicate that the surface architecture of prepared coatings does not affect the main reaction path but have an influence on the reaction rates and yields of observed processes.


Introduction
The design of the architecture of photocatalysts' surfaces in nanoscale is a promising approach to photocatalysis, which enables detailed comprehension of matter behavior [1]. It is known, that the improvement of photocatalytic activity of semiconductors, can be achieved by inter alia defined porosity [2,3], exposition of the selected crystallographic facets [4][5][6], hierarchical structure [7][8][9], decoration with nanoparticles [10,11] and quantum dot incorporation [12][13][14], which enables the limitations of conventional photocatalysts to be overcome. It is believed that the development of multi-component systems can be an effective method for obtaining excellent photocatalysts due to

Preparation of Titanium Dioxide Coatings
Firstly, the silicon substrates were cleaned in a mixture of ethanol and isopropanol in an ultrasonic bath, then with dust-free cloth moistened with ethanol and lastly a stream of compressed air. Titanium dioxide coatings were obtained using the sol-gel method, reported in our previous studies [30,31]. Briefly, titanium tetraisopropoxide and isopropanol with the addition of HCl as a catalyst were stirred for 20 min. Furthermore, prepared sol was applied on silicon wafers substrates using the dip-coating method. Each of the obtained photocatalysts had the same surface area equal to 1 cm 2 . Dipping at the immersion-withdrawal velocity of 25 mm/min was repeated three times with preserving a drying time of 15 min between repetitions. Obtained coatings were annealed at 100 • C and calcined at 500 • C (both for 2 h), leading to obtain anatase phase. 2 Coatings with Graphene Oxide (GO) and Silver Nanostructures (AgNSs) Figure 1 shows a scheme illustrating preparation of two-component and three-component photocatalysts. GO water dispersion in concentration of 0.5 mg/mL was obtained by dilution of stock GO dispersion (2 mg/mL) with deionized water and then, it was used for surface modification of selected coatings (TiO 2 or TiO 2 -AgNSs). GO flakes were transferred onto substrates using dip-coating technique at the immersion-withdrawal velocity of 25 mm/min.

Surface Modification of TiO
Silver nanostructures (AgNSs) on the photocatalysts surfaces were obtained by photoreduction of Ag + ions. Therefore, AgNO 3 ethanol solution at the concentration of 0.1 mM was used as a precursor. Previously prepared coatings (TiO 2 or TiO 2 -GO) were immersed in polymethacrylate (PMMA) cuvettes containing 3.5 mL of AgNO 3 ethanol solution for 5 min, and during this time cuvettes were irradiated with a UV lamp (Consulting Peschl, 2 × 15 W, wavelength λ max = 365 nm, 15 mW/cm 2 ). According to the supplier's specification, selected cuvettes can be applied in the wavelength range from 220 to 900 nm and are transparent at λ max = 365 nm. Subsequently, the coatings were rinsed with deionized water to remove residual ions/solution. On the contrary, the selective decoration of GO sheets deposited on TiO 2 coatings with AgNSs was performed without introducing light, as in method reported previously [32]. Briefly, coatings were immersed in cuvettes with 3.5 mL of AgNO 3 ethanol solution and left in a darkroom for 5 min. After this time coatings also were rinsed with water, as in the case of photoreduction.

Characterization
Morphology of prepared photocatalysts was analyzed using a field-emission scanning electron microscope (FE-SEM-FEI NovaNano SEM 450, FEI, Hillsboro, OR, USA) equipped with a Schottky gun. Images were obtained with the use of the Everhart-Thornley detector (ETD, FEI, Hillsboro, OR, USA) or the through lens detector (TLD, FEI, Hillsboro, OR, USA) in immersion mode. Analysis of surface coverage by GO and AgNSs was estimated using Image J 1.52a software [33].
The diffraction spectra were recorded using an Empyrean PANalytical X-ray diffractometer (XRD, Almelo, Netherlands) equipped with a Co lamp (wavelength λ = 0.1790 nm). Signals were collected in the range of 2θ = 20-120°, using the angle of incidence 0.5° in 0.1° steps. The counting time was 20 sec per step. 2θCo was scaled to the values corresponding to 2θCu using the Rietveld equation in order to compare with the values given in the literature.
Diffuse reflectance spectra were recorded with a UV/Vis diffuse-reflectance spectroscopy (DRS) spectrophotometer PerkinElmer Lambda 25 (Waltham, MA, USA), and band gap energy was determined with the use of Kubelka-Munk equation and Tauc method.

Analysis of Photocatalytic Activity
The photocatalysts obtained were immersed in quartz cuvettes filled with 2.5 mL of rhodamine B (RhB) water solution with a concentration of 1 × 10 −5 M. Before irradiation cuvettes were placed in a dark room for 20 min, receiving a adsorption-desorption equilibrium. During the experiment, cuvettes with air access were placed in front of a xenon lamp (150 W, Instytut Fotonowy, Kraków, Poland) equipped with a UV or Vis cut-off filter, at a distance of 15 cm and 25 cm, respectively. Intensity of radiation was equal to 223 mW/cm 2 in both cases. Changes in RhB spectrum and concentration were monitored using UV-Vis spectrophotometer (USB2000+, Ocean Optics, Dunedin, FL, USA).

Characterization
Morphology of prepared photocatalysts was analyzed using a field-emission scanning electron microscope (FE-SEM-FEI NovaNano SEM 450, FEI, Hillsboro, OR, USA) equipped with a Schottky gun. Images were obtained with the use of the Everhart-Thornley detector (ETD, FEI, Hillsboro, OR, USA) or the through lens detector (TLD, FEI, Hillsboro, OR, USA) in immersion mode. Analysis of surface coverage by GO and AgNSs was estimated using Image J 1.52a software [33].
The diffraction spectra were recorded using an Empyrean PANalytical X-ray diffractometer (XRD, Almelo, Netherlands) equipped with a Co lamp (wavelength λ = 0.1790 nm). Signals were collected in the range of 2θ = 20-120 • , using the angle of incidence 0.5 • in 0.1 • steps. The counting time was 20 sec per step. 2θ Co was scaled to the values corresponding to 2θ Cu using the Rietveld equation in order to compare with the values given in the literature.
Diffuse reflectance spectra were recorded with a UV/Vis diffuse-reflectance spectroscopy (DRS) spectrophotometer PerkinElmer Lambda 25 (Waltham, MA, USA), and band gap energy was determined with the use of Kubelka-Munk equation and Tauc method.

Analysis of Photocatalytic Activity
The photocatalysts obtained were immersed in quartz cuvettes filled with 2.5 mL of rhodamine B (RhB) water solution with a concentration of 1 × 10 −5 M. Before irradiation cuvettes were placed in a dark room for 20 min, receiving a adsorption-desorption equilibrium. During the experiment, cuvettes with air access were placed in front of a xenon lamp (150 W, Instytut Fotonowy, Kraków, Poland) equipped with a UV or Vis cut-off filter, at a distance of 15 cm and 25 cm, respectively. Intensity of radiation was equal to 223 mW/cm 2 in both cases. Changes in RhB spectrum and concentration were monitored using UV-Vis spectrophotometer (USB2000+, Ocean Optics, Dunedin, FL, USA).

Titanium Dioxide Coatings Characterization
Initially, the titanium dioxide coating was prepared using the sol-gel method. In order to obtain TiO 2 in anatase form the calcination process was performed at 500 • C. The crystallographic structure of the coating was verified using X-ray diffraction (XRD). Figure 2 represents a converted diffraction pattern with Miller indices assigned to characteristic anatase peaks. The most characteristic peaks for anatase occur at 2θ values equal to 25.3 • , 37.8 • , 48.1 • , 53.9 • and 55.1 • which correspond to the crystallographic planes: (101), (004), (200), (105) and (211) respectively [34,35]. Since there are no signals in the obtained spectrum, indicating the presence of other crystalline phases, it can be stated that the obtained TiO 2 coating is pure anatase.

Titanium Dioxide Coatings Characterization
Initially, the titanium dioxide coating was prepared using the sol-gel method. In order to obtain TiO2 in anatase form the calcination process was performed at 500 °C. The crystallographic structure of the coating was verified using X-ray diffraction (XRD). Figure 2 represents a converted diffraction pattern with Miller indices assigned to characteristic anatase peaks. The most characteristic peaks for anatase occur at 2θ values equal to 25.3°, 37.8°, 48.1°, 53.9° and 55.1° which correspond to the crystallographic planes: (101), (004), (200), (105) and (211) respectively [34,35]. Since there are no signals in the obtained spectrum, indicating the presence of other crystalline phases, it can be stated that the obtained TiO2 coating is pure anatase. For further characterization of the obtained coating, scanning electron microscopy (SEM) was undertaken. Figure 3a represents a cross-section of the TiO2 layer deposited on the silicon wafer. The average coating thickness is approximately 57 ± 3 nm. The layer is uniformly thick over the entire length. Figure 3b presents the SEM image of the coating surface, which indicates the occurrence of regular porosity with pore sizes not exceeding 2 nm, visible as darker fields. Porosity is the result of the formation of anatase crystal phase during the calcination process, which is distinctive of thin coatings obtained by the sol-gel method [35].  For further characterization of the obtained coating, scanning electron microscopy (SEM) was undertaken. Figure 3a represents a cross-section of the TiO 2 layer deposited on the silicon wafer. The average coating thickness is approximately 57 ± 3 nm. The layer is uniformly thick over the entire length. Figure 3b presents the SEM image of the coating surface, which indicates the occurrence of regular porosity with pore sizes not exceeding 2 nm, visible as darker fields. Porosity is the result of the formation of anatase crystal phase during the calcination process, which is distinctive of thin coatings obtained by the sol-gel method [35].

Titanium Dioxide Coatings Characterization
Initially, the titanium dioxide coating was prepared using the sol-gel method. In order to obtain TiO2 in anatase form the calcination process was performed at 500 °C. The crystallographic structure of the coating was verified using X-ray diffraction (XRD). Figure 2 represents a converted diffraction pattern with Miller indices assigned to characteristic anatase peaks. The most characteristic peaks for anatase occur at 2θ values equal to 25.3°, 37.8°, 48.1°, 53.9° and 55.1° which correspond to the crystallographic planes: (101), (004), (200), (105) and (211) respectively [34,35]. Since there are no signals in the obtained spectrum, indicating the presence of other crystalline phases, it can be stated that the obtained TiO2 coating is pure anatase. For further characterization of the obtained coating, scanning electron microscopy (SEM) was undertaken. Figure 3a represents a cross-section of the TiO2 layer deposited on the silicon wafer. The average coating thickness is approximately 57 ± 3 nm. The layer is uniformly thick over the entire length. Figure 3b presents the SEM image of the coating surface, which indicates the occurrence of regular porosity with pore sizes not exceeding 2 nm, visible as darker fields. Porosity is the result of the formation of anatase crystal phase during the calcination process, which is distinctive of thin coatings obtained by the sol-gel method [35].

Surface Modifications with AgNSs and GO
In order to analyze the impact of photocatalysts architectures on their photocatalytic activity, different TiO 2 surface modifications by GO and AgNSs were obtained. Figure 4 depicts SEM images of prepared photocatalysts and related schemes: two-component coatings: TiO 2 -GO, TiO 2 -AgNSs and three-component coatings: TiO 2 -GO-AgNSs, TiO 2 -(GO-AgNSs) and TiO 2 -AgNSs-GO. Explanation of schemes: white area-TiO 2 thin film, yellow dots-AgNSs, grey objects-GO flakes.

Surface Modifications with AgNSs and GO
In order to analyze the impact of photocatalysts architectures on their photocatalytic activity, different TiO2 surface modifications by GO and AgNSs were obtained. Figure 4 depicts SEM images of prepared photocatalysts and related schemes: two-component coatings: TiO2-GO, TiO2-AgNSs and three-component coatings: TiO2-GO-AgNSs, TiO2-(GO-AgNSs) and TiO2-AgNSs-GO. Explanation of schemes: white area-TiO2 thin film, yellow dots-AgNSs, grey objects-GO flakes. Firstly the TiO2 coatings were used as the substrates for GO deposition. GO sheets were applied on the surface of the photocatalysts using the dip-coating method as described in the experimental section. Figure 4a depict randomly distributed GO flakes on the coating surface, visible as dark objects. Flakes reveal the slight presence of wrinkles, which is characteristic of explicit adhesion to the surface. It was found that GO flakes occupy approximately 50% of the surface of the photocatalyst.
For the purpose of decoration of TiO2 surface with AgNSs, photocatalytic properties of TiO2 were used. During UV irradiation, electrons from the valence band (VB) of TiO2 were transferred to the conduction band (CB), leading to the formation of an electron-hole pair, according to the reaction equation: Photogenerated electrons reduce silver ions adsorbed on TiO2 surface, resulting in silver nanostructures' growth [36]: TiO2 (e − ) + Ag + → TiO2 + Ag 0 (2) At the same time, ethanol acts as a hole scavenger improving the efficiency of photocatalytic growth of AgNSs [37,38]: The SEM image presented in Figure 4c shows representative morphology of obtained TiO2-AgNSs photocatalyst. It can be seen that AgNSs grown on TiO2, visible as white objects, are singleentity and quasi-spherical. The average estimated size of AgNSs was 18 ± 3 nm, and the maximal Firstly the TiO 2 coatings were used as the substrates for GO deposition. GO sheets were applied on the surface of the photocatalysts using the dip-coating method as described in the experimental section. Figure 4a depict randomly distributed GO flakes on the coating surface, visible as dark objects. Flakes reveal the slight presence of wrinkles, which is characteristic of explicit adhesion to the surface. It was found that GO flakes occupy approximately 50% of the surface of the photocatalyst.
For the purpose of decoration of TiO 2 surface with AgNSs, photocatalytic properties of TiO 2 were used. During UV irradiation, electrons from the valence band (VB) of TiO 2 were transferred to the conduction band (CB), leading to the formation of an electron-hole pair, according to the reaction equation: Photogenerated electrons reduce silver ions adsorbed on TiO 2 surface, resulting in silver nanostructures' growth [36]: At the same time, ethanol acts as a hole scavenger improving the efficiency of photocatalytic growth of AgNSs [37,38]: The SEM image presented in Figure 4c shows representative morphology of obtained TiO 2 -AgNSs photocatalyst. It can be seen that AgNSs grown on TiO 2 , visible as white objects, are single-entity and Materials 2020, 13, 4653 7 of 21 quasi-spherical. The average estimated size of AgNSs was 18 ± 3 nm, and the maximal diameter did not exceed 37 nm. The surface density of obtained AgNSs equals 55 AgNSs/µm 2 , and they occupy 1.1% of TiO 2 surface.
In the last step TiO 2 coatings modified with both GO and AgNSs were received. Since it was assumed that the way of combining the components could have a significant impact on the photocatalytic properties of the composites, three types of photocatalysts were prepared: TiO 2 -AgNSs-GO, TiO 2 -GO-AgNSs and TiO 2 -(GO-AgNSs). To obtain TiO 2 -AgNSs-GO composite, a previously obtained TiO 2 -AgNSs photocatalyst was used as a substrate for dip-coating deposition of GO flakes. Whereas previously received TiO 2 -GO coatings were used for preparation of TiO 2 -GO-AgNSs and TiO 2 -(GO-AgNSs). In the first case TiO 2 -GO was immersed in AgNO 3 ethanol solution and irradiated with UV light at the same conditions as in preparation of TiO 2 -AgNSs mentioned above, resulting in coverage of TiO 2 and GO by AgNSs (Figure 4d). By contrast, for the purpose of  Figure 4d-f, confirm that these coatings differ in the distribution of AgNSs (Table 1), which is the result of the preparation method. In the case of TiO 2 -GO-AgNSs surface, AgNSs are visible on both uncovered TiO 2 and covered by GO. Here, the growth of AgNSs was stimulated by photogenerated electrons from the excited TiO 2 surface. By contrast, AgNSs were grown only on the GO sheets on TiO 2 -(GO-AgNSs) surface. Growth of AgNSs on GO was possible due to chemical properties of this material [32,39,40]. In our previous study [32] it was proved that the presence of oxygen functional groups on the graphene oxide surface provides reactive sites for the spontaneous chemical reduction of Ag + ions, leading to formation of AgNSs. It was found that hydroxyl groups were mainly responsible for AgNSs' nucleation. These results were observed after immersion of GO deposited on Si substrate in AgNO 3 ethanol solution carried out in a darkroom. The conditions of this experiment were consistent with those in the present work. Taking a closer look at the characteristic parameters of AgNSs, certain differences can be observed comparing the results obtained for Si-GO-AgNSs [32] with TiO 2 -(GO-AgNSs). The AgNSs size (3 ± 2 nm, max 20 nm) found on Si-(GO-AgNSs) is smaller than that noted on TiO 2 -(GO-AgNSs)-average size 19 ± 3 nm, max 53 nm. Simultaneously, surface density for Si-(GO-AgNSs) which equals to 203 AgNSs/µm 2 is definitely larger than that for TiO 2 -(GO-AgNSs)-3 AgNSs/µm 2 . The reason for these differences is related to the nature of the applied substrate. Presumably, hydroxyl groups from GO interact more intensely with hydroxyl groups localized on TiO 2 surface than on Si. Consequently, most of the GO hydroxyl groups are involved in creating interactions with the TiO 2 surface. This results in fewer free functional groups, providing less nucleation sites for AgNSs growth, which translates further into their larger sizes.
When the generation of AgNSs is performed under UV irradiation, the surface decoration turns out different. Analyzing TiO 2 -GO-AgNSs surface coverage, where the AgNSs growth was stimulated by the participation of UV irradiation, almost 12 times more AgNSs (35 AgNSs/µm 2 ) were formed on GO flakes than on flakes deposited on the TiO 2 -(GO-AgNSs), where the modification was carried out without an access of light ( Figure 5). At the same time as the AgNSs number increases, the resulting nanostructures are also characterized by larger sizes-the maximum size increased from 53 nm to 66 nm, and the average size from 19 ± 3 nm to 26 nm ± 4. This is clear evidence that the growth process was stimulated by another factor. Lightcap and co-authors [38] proved that titanium dioxide excited by UV irradiation transfers an electron to GO, which then migrates inside the flake to adsorbed Ag + ions on its surface, resulting in their reduction to metallic silver. On this basis, it can be concluded that electrons photoinduced in TiO 2 are involved in AgNSs growth on the GO deposited on the TiO 2 surface. Furthermore, this theory can be supported by the results of AgNSs photogeneration on the uncovered TiO 2 surface in TiO 2 -GO-AgNSs coating in comparison with TiO 2 -AgNSs ( Figure 6). The size of obtained AgNSs on both surfaces are similar, but the AgNSs surface density on the TiO 2 area covered by GO in TiO 2 -GO-AgNSs is almost 2.75 times smaller. This phenomenon can be elucidated by the possibility that photogenerated electrons in TiO 2 -GO, which could take part in reduction of Ag + on TiO 2 , are trapped in GO resulting in reduction of AgNSs surface density on the TiO 2 surface in TiO 2 -GO-AgNSs composite compared to TiO 2 -AgNSs. results in fewer free functional groups, providing less nucleation sites for AgNSs growth, which translates further into their larger sizes.
When the generation of AgNSs is performed under UV irradiation, the surface decoration turns out different. Analyzing TiO2-GO-AgNSs surface coverage, where the AgNSs growth was stimulated by the participation of UV irradiation, almost 12 times more AgNSs (35 AgNSs/µm 2 ) were formed on GO flakes than on flakes deposited on the TiO2-(GO-AgNSs), where the modification was carried out without an access of light ( Figure 5). At the same time as the AgNSs number increases, the resulting nanostructures are also characterized by larger sizes-the maximum size increased from 53 nm to 66 nm, and the average size from 19 ± 3 nm to 26 nm ± 4. This is clear evidence that the growth process was stimulated by another factor. Lightcap and co-authors [38] proved that titanium dioxide excited by UV irradiation transfers an electron to GO, which then migrates inside the flake to adsorbed Ag + ions on its surface, resulting in their reduction to metallic silver. On this basis, it can be concluded that electrons photoinduced in TiO2 are involved in AgNSs growth on the GO deposited on the TiO2 surface. Furthermore, this theory can be supported by the results of AgNSs photogeneration on the uncovered TiO2 surface in TiO2-GO-AgNSs coating in comparison with TiO2-AgNSs ( Figure 6). The size of obtained AgNSs on both surfaces are similar, but the AgNSs surface density on the TiO2 area covered by GO in TiO2-GO-AgNSs is almost 2.75 times smaller. This phenomenon can be elucidated by the possibility that photogenerated electrons in TiO2-GO, which could take part in reduction of Ag + on TiO2, are trapped in GO resulting in reduction of AgNSs surface density on the TiO2 surface in TiO2-GO-AgNSs composite compared to TiO2-AgNSs.   results in fewer free functional groups, providing less nucleation sites for AgNSs growth, which translates further into their larger sizes.
When the generation of AgNSs is performed under UV irradiation, the surface decoration turns out different. Analyzing TiO2-GO-AgNSs surface coverage, where the AgNSs growth was stimulated by the participation of UV irradiation, almost 12 times more AgNSs (35 AgNSs/µm 2 ) were formed on GO flakes than on flakes deposited on the TiO2-(GO-AgNSs), where the modification was carried out without an access of light ( Figure 5). At the same time as the AgNSs number increases, the resulting nanostructures are also characterized by larger sizes-the maximum size increased from 53 nm to 66 nm, and the average size from 19 ± 3 nm to 26 nm ± 4. This is clear evidence that the growth process was stimulated by another factor. Lightcap and co-authors [38] proved that titanium dioxide excited by UV irradiation transfers an electron to GO, which then migrates inside the flake to adsorbed Ag + ions on its surface, resulting in their reduction to metallic silver. On this basis, it can be concluded that electrons photoinduced in TiO2 are involved in AgNSs growth on the GO deposited on the TiO2 surface. Furthermore, this theory can be supported by the results of AgNSs photogeneration on the uncovered TiO2 surface in TiO2-GO-AgNSs coating in comparison with TiO2-AgNSs ( Figure 6). The size of obtained AgNSs on both surfaces are similar, but the AgNSs surface density on the TiO2 area covered by GO in TiO2-GO-AgNSs is almost 2.75 times smaller. This phenomenon can be elucidated by the possibility that photogenerated electrons in TiO2-GO, which could take part in reduction of Ag + on TiO2, are trapped in GO resulting in reduction of AgNSs surface density on the TiO2 surface in TiO2-GO-AgNSs composite compared to TiO2-AgNSs.    [41]. The arrangement of GO flakes can produce two effects. On the one hand any type of deformation in the structure of graphene materials has a negative impact on electrons' movement in its structure. While on the other hand, the appearance of wrinkles allows the solution to penetrate between the surface of the photocatalyst and the GO flake, which can be advantageous from the viewpoint of photocatalysis.
A further characteristic of photocatalytic systems was performed by diffuse-reflectance spectroscopy (DRS). Figure 7 shows a graph which depicts the dependence of the Tauc function on the photon energy (F(KM/α)hν) 1 2 = f(hν) for TiO 2 , TiO 2 -GO and TiO 2 -AgNSs coatings. The determined value of bandgap energy (E g ) for these coatings equals 3.2 eV, which is typical of the anatase form of TiO 2 [19,42]. The presence of AgNSs and GO on the TiO 2 surface did not change the value of the semiconductor E g . The plot obtained for TiO 2 -AgNSs shows that localized surface plasmon resonance (LSPR) is not observed. This means that all changes in photocatalytic properties of obtained coatings, gained after modification with AgNSs and GO, were not caused by differences in E g value. TiO2, and the AgNSs that are formed on them do not change the arrangement of flakes and their adhesion to the substrate. These flakes show only local multiplication of the GO layer as in the TiO2-GO coating described earlier. By contrast, in the case of TiO2-AgNSs-GO, where GO was deposited on previously grown silver nanostructures, small wrinkles are visible (in the form of characteristic white "lines" between AgNSs). Presence of AgNSs under GO flakes effects in surface unevenness, which increase the tendency of GO to wrinkling [41]. The arrangement of GO flakes can produce two effects. On the one hand any type of deformation in the structure of graphene materials has a negative impact on electrons' movement in its structure. While on the other hand, the appearance of wrinkles allows the solution to penetrate between the surface of the photocatalyst and the GO flake, which can be advantageous from the viewpoint of photocatalysis. A further characteristic of photocatalytic systems was performed by diffuse-reflectance spectroscopy (DRS). Figure 7 shows a graph which depicts the dependence of the Tauc function on the photon energy (F(KM/α)hν)½ = f(hν) for TiO2, TiO2-GO and TiO2-AgNSs coatings. The determined value of bandgap energy (Eg) for these coatings equals 3.2 eV, which is typical of the anatase form of TiO2 [19,42]. The presence of AgNSs and GO on the TiO2 surface did not change the value of the semiconductor Eg. The plot obtained for TiO2-AgNSs shows that localized surface plasmon resonance (LSPR) is not observed. This means that all changes in photocatalytic properties of obtained coatings, gained after modification with AgNSs and GO, were not caused by differences in Eg value.

Photocatalytic Transformations of Rhodamine B
The evaluation of photocatalytic properties of the obtained photocatalysts was performed by the spectrophotometric observation of changes in the RhB solution spectrum during irradiation. Experiments were carried out with aqueous solution of RhB in two ranges of light: UV and Vis. Two different phenomena were studied-a direct activation of photocatalyst and sensitization. On the one hand, UV light activate TiO2, providing photogeneration of hydroxyl radicals ( • OH) and other reactive forms of oxygen. These species react with the RhB molecules leading to their decomposition [43,44]. On the other hand, Vis light does not excite TiO2, but can affect the RhB molecules leading to their excitation. Then, oxygen radicals arise on TiO2 by indirect sensitization process, after the transfer of electrons from lowest unoccupied molecular orbital (LUMO) of RhB molecules in excited state to the conduction band of TiO2 [45]. This process is possible due to the fact, that the LUMO energy level

Photocatalytic Transformations of Rhodamine B
The evaluation of photocatalytic properties of the obtained photocatalysts was performed by the spectrophotometric observation of changes in the RhB solution spectrum during irradiation. Experiments were carried out with aqueous solution of RhB in two ranges of light: UV and Vis. Two different phenomena were studied-a direct activation of photocatalyst and sensitization. On the one hand, UV light activate TiO 2 , providing photogeneration of hydroxyl radicals ( • OH) and other reactive forms of oxygen. These species react with the RhB molecules leading to their decomposition [43,44]. On the other hand, Vis light does not excite TiO 2 , but can affect the RhB molecules leading to their excitation. Then, oxygen radicals arise on TiO 2 by indirect sensitization process, after the transfer of electrons from lowest unoccupied molecular orbital (LUMO) of RhB molecules in excited state to the conduction band of TiO 2 [45]. This process is possible due to the fact, that the LUMO energy level of rhodamine B is higher (−2.73 eV) [45] than the lower edge of the anatase conduction band (−4.0 to −4.3 eV) [46], and is widely applied in the field of dye-sensitized solar cells (DSSC's) and also in photocatalysis [47,48].
These two mechanisms of excitation result in different pathways of RhB decomposition. Figures 8  and 9 contain compiled graphs, presenting the changes in absorption spectrum of RhB under UV and Vis light irradiation in the presence of bare TiO 2 coating, respectively. In the case of UV irradiation, a decrease in the height of peak around 554 nm is observed without any significant changes in peaks positions, which is typical phenomenon for chromophore destruction in the process of RhB photodegradation. Measurement of absorbance value at the wavelength 554 nm were used for determination of reaction rate constant (k') based on Langmuir-Hinshelwood's model following the pseudo-first-order kinetics expressed as [49]: where: k' is the pseudo-first-order rate constant (min −1 ), C 0 the initial concentration of RhB and C is the concentration of RhB at the time t. This methodology is often used in the case of estimation of photocatalyst activity in dye photodecomposition [25,[50][51][52][53][54].
Materials 2020, 11, x FOR PEER REVIEW 10 of 21 of rhodamine B is higher (−2.73 eV) [45] than the lower edge of the anatase conduction band (−4.0 to −4.3 eV) [46], and is widely applied in the field of dye-sensitized solar cells (DSSC's) and also in photocatalysis [47,48]. These two mechanisms of excitation result in different pathways of RhB decomposition. Figures  8 and 9 contain compiled graphs, presenting the changes in absorption spectrum of RhB under UV and Vis light irradiation in the presence of bare TiO2 coating, respectively. In the case of UV irradiation, a decrease in the height of peak around 554 nm is observed without any significant changes in peaks positions, which is typical phenomenon for chromophore destruction in the process of RhB photodegradation. Measurement of absorbance value at the wavelength 554 nm were used for determination of reaction rate constant (k') based on Langmuir-Hinshelwood's model following the pseudo-first-order kinetics expressed as [49]: where: k' is the pseudo-first-order rate constant (min −1 ), C0 the initial concentration of RhB and C is the concentration of RhB at the time t. This methodology is often used in the case of estimation of photocatalyst activity in dye photodecomposition [25,[50][51][52][53][54].   Materials 2020, 11, x FOR PEER REVIEW 10 of 21 of rhodamine B is higher (−2.73 eV) [45] than the lower edge of the anatase conduction band (−4.0 to −4.3 eV) [46], and is widely applied in the field of dye-sensitized solar cells (DSSC's) and also in photocatalysis [47,48]. These two mechanisms of excitation result in different pathways of RhB decomposition. Figures  8 and 9 contain compiled graphs, presenting the changes in absorption spectrum of RhB under UV and Vis light irradiation in the presence of bare TiO2 coating, respectively. In the case of UV irradiation, a decrease in the height of peak around 554 nm is observed without any significant changes in peaks positions, which is typical phenomenon for chromophore destruction in the process of RhB photodegradation. Measurement of absorbance value at the wavelength 554 nm were used for determination of reaction rate constant (k') based on Langmuir-Hinshelwood's model following the pseudo-first-order kinetics expressed as [49]: where: k' is the pseudo-first-order rate constant (min −1 ), C0 the initial concentration of RhB and C is the concentration of RhB at the time t. This methodology is often used in the case of estimation of photocatalyst activity in dye photodecomposition [25,[50][51][52][53][54].   However, for the determination of photocatalyst activity under Vis light irradiation, reaction rate constant parameter is not sufficient. Analysis of the graph presented in Figure 9 indicates two processes occurring simultaneously. During the elongation of exposure to Vis light, the initial absorbance value at the maximum of peak at the wavelength 554 nm decrease. At the same time the hypsochromic shift can be seen, and after 280 min of the photocatalytic process the peak with the maximum at 498 nm is extracted. After 280 min, the spectrum does not undergoes any changes. The peak with maximum at 498 nm was identified as a signal from rhodamine 110 (Rh-110) which is similar to results obtained in studies of photocatalytic transformation of rhodamine B in the presence of TiO 2 [55][56][57], TiO 2 -Ag [55], TiO 2 -Si [57], CdS [55,58], Pb 3 Nb 4 O 13 [59] irradiated by Vis light. The same effects were observed during photocatalytic measurements performed under Vis irradiation for every prepared type of coating analyzed in this study.
The process of photocatalytic transformation of RhB into Rh-110 via the N-deethylation mechanism was firstly described by Watanabe et al. [58]. In this process, ethyl groups are eliminated from the aminodiethyl groups of RhB, resulting in consecutively formation of N,N,N'-triethyl-Rh-110, N,N'-diethyl-Rh-110, N-ethyl-Rh-110 and Rh-110. These compounds have absorption maxima at the wavelength of 539 nm, 522 nm, 510 nm and 498 nm, respectively. Ethyl groups in RhB molecules structure act as the auxochromes, determining the location of the absorption maximum. Their elimination cause the hypsochromic shift shown in the spectrum. It was found that during elimination of ethyl groups from the adsorbed dye on photocatalyst surface, the excess negative charge accumulated on TiO 2 is removed by the adsorbed oxygen molecule, from which the superoxide radical is formed [59]. In that case indirect sensitization affect the reaction path of reactive oxygen species (ROS) generation, promoting formation of O 2 •− and decreasing probability of • OH production.
To the best of our knowledge, the procedure for quantitative determination of the photocatalytic conversion of rhodamine B into rhodamine 110 under visible light irradiation has not been described in literature yet. In order to perform the mathematical estimation of this phenomenon, we propose in our study determination of conversion efficiency (W c ) factor. This parameter is defined by the ratio of the actual number of moles (n a ) of the substance obtained as a result of chemical transformation, to the theoretical number of moles (n t ) of this substance that would be obtained as a result of this reaction assuming that all the substrate molecules were converted into product. Conversion efficiency is described by the formula: Due to the fact that the chemical transformation of RhB into Rh-110 takes place in the same volume, the number of moles can be converted to molar concentration. After using the Bouguer-Lambert-Beer law, the formula takes the form: In order to make the appropriate calculations, the molar extinction coefficient (ε) for RhB and Rh-110 was estimated experimentally. It was found ε RhB equals 89 590 cm −1 M −1 and ε Rh-110 equals 70 605 cm −1 M −1 . In the present study conversion coefficient has been calculated using value of A RhB at the peak maximum at the wavelength 554 nm presented by initial RhB solution (with concentration 1 × 10 −5 M) and A Rh-110 at the peak maximum at the wavelength 498 nm measured after 300 min of photocatalytic process.
Determination of conversion efficiency allows also the calculation of removal efficiency (W r ): Removal efficiency describes photocatalytical degradation of RhB molecules, as a result of chromophore destruction.
Conversion efficiency or removal efficiency cannot be considered separately in studies of photocatalytic performance, but should always be analyzed together with the reaction rate constant. Observed processes can be analyzed in terms of the contaminant removal or synthesis of the intended compound.

Analysis of Photocatalytic Properties
Results of the photocatalytic transformations of RhB by different photocatalysts under UV and Vis irradiation are shown in Figures 10 and 11, respectively. Estimated reaction rates and conversion efficiency related to photocatalytic activity of obtained TiO 2 , TiO 2 -GO, TiO 2 -AgNSs, TiO 2 -AgNSs-GO, TiO 2 -GO-AgNSs and TiO 2 -(GO-AgNSs) coatings under UV and Vis irradiation are presented in Table 2.
The results clearly indicate that photocatalytic activity depends on the composition and architecture of the coating. Observed processes can be analyzed in terms of the contaminant removal or synthesis of the intended compound.

Analysis of Photocatalytic Properties
Results of the photocatalytic transformations of RhB by different photocatalysts under UV and Vis irradiation are shown in Figures 10 and 11, respectively. Estimated reaction rates and conversion efficiency related to photocatalytic activity of obtained TiO2, TiO2-GO, TiO2-AgNSs, TiO2-AgNSs-GO, TiO2-GO-AgNSs and TiO2-(GO-AgNSs) coatings under UV and Vis irradiation are presented in Table  2. The results clearly indicate that photocatalytic activity depends on the composition and architecture of the coating.

Under UV Irradiation
Involving GO and AgNSs in the photocatalytic system leads to an increase of its activity in the RhB degradation under UV irradiation. In binary systems, the incorporation of AgNSs is more efficient (0.0352 min −1 ) than deposition of GO flakes (0.0256 min −1 ). A high activity of TiO2-AgNSs coatings is the result of electrons trapping by the Schottky junction and the possibility of generation of the hydroxyl radicals on the AgNSs surfaces [18].
GO combined with TiO2 also acts as an electron sink, resulting in delay in recombination of electron-hole pair [60], but the behavior of this system under UV is more complex. It is known that without access of oxygen GO can be photoreduced on TiO2 by excited electron from CB, leading to reconstruction of a conjugated network [61], but with access of air this reaction path is interrupted by a competitive process of oxidation of oxygen moieties localized in a GO structure, which leads to the decomposition of flakes [21,22]. This process depends on the intensity of radiation, and thereby reactive oxygen species production. Moreover, residual oxygen moieties on reduced graphene oxide (RGO) can undergo oxidation by superoxide anion [62]. Herein, the amount of GO in all coatings was

Under UV Irradiation
Involving GO and AgNSs in the photocatalytic system leads to an increase of its activity in the RhB degradation under UV irradiation. In binary systems, the incorporation of AgNSs is more efficient (0.0352 min −1 ) than deposition of GO flakes (0.0256 min −1 ). A high activity of TiO 2 -AgNSs coatings is the result of electrons trapping by the Schottky junction and the possibility of generation of the hydroxyl radicals on the AgNSs surfaces [18].
GO combined with TiO 2 also acts as an electron sink, resulting in delay in recombination of electron-hole pair [60], but the behavior of this system under UV is more complex. It is known that without access of oxygen GO can be photoreduced on TiO 2 by excited electron from CB, leading to reconstruction of a conjugated network [61], but with access of air this reaction path is interrupted by a competitive process of oxidation of oxygen moieties localized in a GO structure, which leads to the decomposition of flakes [21,22]. This process depends on the intensity of radiation, and thereby reactive oxygen species production. Moreover, residual oxygen moieties on reduced graphene oxide (RGO) can undergo oxidation by superoxide anion [62]. Herein, the amount of GO in all coatings was identical, which eliminates the impact of the aforementioned phenomena on the comparison of various architectures.
TiO 2 -AgNSs-GO coating shows the best photocatalytic properties in UV light among all the coatings examined in this work. The value of the constant rate of RhB degradation on this coating (0.0405 min −1 ) is almost 2 times higher (exactly 98% higher) the value of the rate constant for unmodified TiO 2 coating (0.0204 min −1 ). Interestingly, deposition of GO flakes (TiO 2 -GO; 0.0256 min −1 ) leads also to an increase of the reaction rate constant value of unmodified TiO 2 , but only by 25%. However, decoration of TiO 2 by AgNSs resulting in the TiO 2 -AgNSs photocatalyst (which differs from TiO 2 -AgNSs-GO coating only by the absence of GO flakes on the surface) leads to an increase of this value by 72%. On this basis, it can be concluded that the additive effect increasing the photocatalytic performance of both components (i.e., AgNSs and GO) occurs in the TiO 2 -AgNSs-GO coating. Most likely, this effect is related to the behavior of AgNSs as electron traps, resulting in the suppressing of electron-hole recombination. Furthermore, it is also possible that, due to the fact that GO flakes are located on AgNSs, electrons can be transferred from AgNSs to the GO structure, which causes even greater delay of the recombination process.
The presence of silver and GO appeared also beneficial in other types of architecture. The TiO 2 -(GO-AgNSs) coating (0.0331 min −1 ) differs from the TiO 2 -GO coating (0.0256 min −1 ) only by the presence of AgNSs on the surface of GO flakes. The introduction of AgNSs has further improved the process of photocatalytic decolorization of RhB. The value of the reaction rate constant on the TiO 2 -(GO-AgNSs) coating is 62% higher than the value for the unmodified coating. Compared to TiO 2 -GO, the introduction of AgNSs increased the reaction rate constant by 37%. In the TiO 2 -(GO-AgNSs) coating, the interaction of both components is also revealing, leading to the acceleration of the photocatalytic degradation of RhB in UV light.
In contrast, the TiO 2 -GO-AgNSs (0.0309 min −1 ), which is characterized by areas covered or uncovered with GO flakes, differing in the number and size of AgNSs, also shows an improvement in photocatalytic properties in comparison with TiO 2 -GO. However, the value of the increase of the reaction rate constant is not so high-only 26%. It is worth noting, that for the TiO 2 -(GO-AgNSs), the value of the reaction rate constant compared to TiO 2 -GO was 37% higher and is more than 11% higher than for TiO 2 -GO-AgNSs. Therefore, the AgNSs localized on the TiO 2 surface not covered with GO flakes may provoke competitive phenomena. The excited electron from TiO 2 can be transferred both to AgNSs situated on TiO 2 or to AgNSs connected with GO.
The discussed phenomena occurring in the presence of three-component coatings under the UV radiation are presented in Figure 12. To summarize the experiments conducted under UV irradiation, it was found that the incorporation of both GO and AgNSs with TiO2 leads to enhancement of photocatalytic degradation of RhB. The architecture of the ternary coating intensively affects the photocatalyst activity resulting in significant differences in constant rate values. However, it should be taken into consideration that GO flakes deposited on TiO2 surface under that range of irradiation are prone to decompose, which ultimately means that the photocatalysts including them are not stable in that condition. In that case, a strategy to combine TiO2 only with AgNSs seem to be more beneficial for the photocatalysts' applications under UV irradiation. To summarize the experiments conducted under UV irradiation, it was found that the incorporation of both GO and AgNSs with TiO 2 leads to enhancement of photocatalytic degradation of RhB. The architecture of the ternary coating intensively affects the photocatalyst activity resulting in significant differences in constant rate values. However, it should be taken into consideration that GO flakes deposited on TiO 2 surface under that range of irradiation are prone to decompose, which ultimately means that the photocatalysts including them are not stable in that condition. In that case, a strategy to combine TiO 2 only with AgNSs seem to be more beneficial for the photocatalysts' applications under UV irradiation.

Under Visible Light (Vis) Irradiation
By contrast with the processes observed in the UV range, under visible light irradiation, the RhB degradation is processing simultaneously with its transformation into Rh-110. As it was mentioned above, the process of N-deethylation is associated with the adsorption process of the dye on the TiO 2 surface.
It is known that GO is the preferred area for adsorption of RhB molecules by π-π stacking interactions [64]. Moreover, GO that covers the TiO 2 surface results in competitive adsorption of RhB on GO rather than on semiconductor surface leading to lowering of interactions of the dye with the semiconductor surface via aminoethyl groups [59]. Consequently, this decreases the probability of electron injection from RhB to TiO 2 , which is necessary under Vis irradiation to provide sensitization of TiO 2 . In that case, RhB is not efficiently transformed into Rh-110. Even when the electron transfer occurs, the electron from CB in TiO 2 can be effectively transported to GO leading to its reduction [61]. However, superoxide radical produced during the RhB N-deethylation process may promote GO oxidation. It is probable that reactive oxygen species and products that arose during GO oxidation can interact with RhB molecules, which promotes chromophore degradation. Therefore, the transformation of RhB to Rh-110 is limited (conversion efficiency valued 53%), but its degradation is accelerated (0.0095 min −1 ).
AgNSs deposited on TiO 2 cover only 1.1% of the surface, so decreasing the area for adsorption of RhB is negligible. Moreover, AgNSs promote transformation of RhB to Rh-110 by electron trapping, through the Schottky junction, which results in the increase of conversion efficiency to 67% in contrast with bare TiO 2 . Electrons trapped in metallic centers (AgNSs) react with adsorbed oxygen leading to the appearance of superoxide radical • O 2¯t hat promotes the transformation of RhB into Rh-110. Therefore, degradation of chromophore is limited, and simultaneously overall process is decelerated. In that case, the value of rate constant for RhB degradation on TiO 2 -AgNS is almost two times lower in comparison with unmodified TiO 2 .
Opposite mechanisms resulting from addition of AgNSs and GO affect the activity of ternary systems simultaneously.
The TiO 2 -(GO-AgNSs) has similar photocatalytic activity to TiO 2 -GO under Vis irradiation. The value of the conventional reaction rate constant for the process carried out on TiO 2 -(GO-AgNSs) equal to 0.0102 min −1 is only slightly higher than the rate constant for TiO 2 -GO (0.0095 min −1 ). Equally determined values of the efficiency of the RhB transformation process in Rh-110 are comparable-52% for TiO 2 -(GO-AgNSs) and 53% for TiO 2 -GO. Therefore, it can be concluded that the additional presence of AgNSs in three-component system, has slight effect on the photocatalytic transformation of RhB into Rh-110, but the addition of GO has a dominant effect.
The properties of the TiO 2 -AgNSs-GO coating should be compared with both TiO 2 -GO and TiO 2 -AgNSs. In a two-component system, the addition of GO caused an increase in the value of a constant reaction rate, while the addition of AgNSs caused a decrease. Both of these phenomena were reflected in the properties of the TiO 2 -AgNSs-GO coating. Their opposite effects caused the conventional reaction rate constant for TiO 2 -AgNSs-GO (0.0082 min −1 ) to be slightly lower than the value characterizing unmodified TiO 2 (0.0088 min −1 ). In addition, the determined yield value of 60% was similar to the value determined for unmodified TiO 2 (65%). To sum up, the effects from AgNSs and GO eliminate each other.
TiO 2 -GO-AgNSs coating is covered with AgNSs to a greater extent than TiO 2 -AgNSs-GO. Therefore, a decrease in the reaction rate constant value to 0.0053 min −1 is visible. This value is similar to the value obtained for the TiO 2 -AgNSs coating (0.0047 min −1 ). The determined efficiency of the RhB transformation process in Rh-110 equal to 55% is much lower than for the TiO 2 -AgNSs coating (67%), but also it is slightly higher than for the TiO 2 -GO coating (53%). Therefore, in the case of TiO 2 -GO-AgNSs coating, the effect of deceleration of the process of RhB photocatalytic transformation resulting from the addition of AgNSs and a decrease in this process efficiency resulting from the addition of GO can be observed.
The discussed phenomena occurring in the presence of three-component coatings under the UV and Vis radiation are presented in Figure 13. To summarize the Vis experiments, GO exerts a dominant effect on the efficiency of photocatalytic conversion of RhB into Rh-110 in all cases, and also increases the degradation of RhB. By contrast, decoration of TiO2 by AgNSs leads to prolongation of the photocatalytic transformation of RhB. However, a small addition of AgNSs located on GO flakes causes a slight acceleration of the process. These observations are in good agreement with the effect of AgNSs electron trapping, elucidated in the mechanism presented by Liu et al. [24].

Conclusions
This work provides a comprehensive study on ternary TiO2 coatings with GO and AgNSs and unravels which components affect the photocatalytic properties of the final materials. Received data indicate that the influence of both modifications is significant and differ under particular range of light. The impact of the AgNSs contribution is rather complex. Decoration with AgNSs leads to higher reaction rate constants in the UV radiation range, whereas under Vis irradiation it elongates decomposition of RhB improving at the same time RhB conversion efficiency. By contrast, the presence of GO increases the decomposition rate of RhB in both selected ranges of radiation. Under Vis illumination, the impact of GO in ternary systems is usually dominant. A synergistic effect of To summarize the Vis experiments, GO exerts a dominant effect on the efficiency of photocatalytic conversion of RhB into Rh-110 in all cases, and also increases the degradation of RhB. By contrast, decoration of TiO 2 by AgNSs leads to prolongation of the photocatalytic transformation of RhB. However, a small addition of AgNSs located on GO flakes causes a slight acceleration of the process. These observations are in good agreement with the effect of AgNSs electron trapping, elucidated in the mechanism presented by Liu et al. [24].

Conclusions
This work provides a comprehensive study on ternary TiO 2 coatings with GO and AgNSs and unravels which components affect the photocatalytic properties of the final materials. Received data indicate that the influence of both modifications is significant and differ under particular range of light. The impact of the AgNSs contribution is rather complex. Decoration with AgNSs leads to higher reaction rate constants in the UV radiation range, whereas under Vis irradiation it elongates decomposition of RhB improving at the same time RhB conversion efficiency. By contrast, the presence of GO increases the decomposition rate of RhB in both selected ranges of radiation. Under Vis illumination, the impact of GO in ternary systems is usually dominant. A synergistic effect of both components is not observed due to favoritism of opposite processes under the applied conditions. Only in the case of TiO 2 -GO-AgNSs architecture under UV irradiation the synergism of both modifications influencing the degradation of RhB was observed. Hence, this work indicates that architecture of photocatalyst surface has huge impact on its photocatalytic activity and this impact can differ in selected range of radiation.
Moreover, phenomena which occur during photochemical processes involving RhB were discussed. It was found that under UV irradiation RhB undergoes only photodegradation, while in the visible light range its transformation into rhodamine 110 (Rh-110) is preferred. This can be explained by the fact that UV irradiation causes the appearance of • OH radicals that decompose RhB by the oxidation path. In the case of the Vis range, the formation of superoxide radical • O 2 − , that can be responsible for promotion of chemical transformation of RhB to Rh-110, is favored. Further conversion of • O 2 − to • OH may also occur which leads to RhB mineralization [55]. However, transformation into Rh-110 prevails. A simple and novel method for the estimation of the photocatalytic activity in terms of transformation of RhB into Rh-110 was proposed.
Most of the actual studies focus on examining the effectiveness of photocatalytic systems in artificial solar light conditions, due to striving to conduct the process with the use of our natural energy source. In the presented work, it was indicated that the processes occurring in the selected range of light can have different reaction paths, which can interrupt each other under solar light irradiation. That phenomenon should be taken into consideration when designing photocatalysts for tailored applications.