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Visible-light-driven photocatalytic degradation of safranin-T dye using functionalized graphene oxide nanosheet (FGS)/ZnO nanocomposites

Photocatalysts suffer from a lack of separation of photogenerated excitons due to the fast recombination of charge carriers, so a strong synergistic effect exhibited by photocatalysts is promising for effective photocatalysis. Herein, we have synthesized efficient visible light functionalized graphene oxide nanosheet (FGS)/ZnO nanocomposite photocatalysts via a simple and economical approach with large scale production for practical applications. A series of nanocomposites (FGS/ZnO NCs) with different amounts by weight of graphene oxide (GO) have been synthesized via a facile solution route followed by calcination under environmental conditions. The phase, purity and morphological studies of the synthesized FGS/ZnO NCs were carried out using powder X-ray diffraction (XRD) and transmission electron microscopy (TEM). The optical properties were studied using UV-visible diffuse reflectance spectroscopy (DRS) and photoluminescence spectroscopy (PL). XRD results confirm the formation of a pure phase of ZnO in the FGS/ZnO NCs and TEM results show strongly adhered ZnO NPs on the surface of the FGS. DRS results confirm the extension of light absorption in the visible region while PL results confirm the effective separation of charge carriers in 0.09 wt% FGS/ZnO NCs. The synthesized photocatalyst efficiently degrades carcinogenic safranin-T dye under visible light illumination which is reported for the first time using FGS/ZnO nanocomposites. Photocatalytic studies confirm the higher photocatalytic activity of 0.09 wt% FGS/ZnO NCs (about 94.5%) towards the photodegradation of safranin-T dye in aqueous solution under visible light. The improved photocatalytic activity of 0.09 wt% FGS/ZnO NCs can be ascribed to the integrative synergistic effects of the enhanced adsorption capacity of safranin-T dye, effective separation of photogenerated excitons and effective interfacial hybridization of FGS and ZnO NCs. The generation of reactive oxygen species was confirmed using terephthalic acid as a probe molecule and a scavenger test was conducted in presence of histidine.


Introduction
In the current decade, photocatalysis using either visible light or solar light has become one of the hot research areas due to alarming levels of global warming caused by various industrial pollutants. [1][2][3] Organic dyes and their effluents have become the main sources of water contamination, which generally originate from many industries such as textile, paper, plastic, etc. Among them, textile industries are signicant consumers of various organic dyes and release waste effluents into aqueous streams. 4,5 In the catalogue of harmful dyes, azo dyes are commonly used in various industries and their associated colour in wastewater is quite noticeable, and they are proven to be potentially carcinogenic and teratogenic to aquatic life as well as the public. [4][5][6] These azo dyes are easily water-soluble and difficult to remove or degrade due to their high solubility, stability and the composition ratio of the aromatic rings in their molecular structure. Most of the azo dyes are known to be largely non-biodegradable in aerobic conditions and they are also photochemically active. 6,7 Therefore, huge research efforts have been devoted to destroying them efficiently in aqueous systems or dispersion systems using UV and solar light. Photocatalysis using UV active semiconductors is quite difficult due to its limited use of the solar spectrum. Additionally, photocatalysis using visible-light-active heteronanostructured semiconductors has shown remarkable progress due to its ease of operation, feasibility, reproducibility, reliability, commercialization, etc. [8][9][10][11] Photocatalytic degradation of organic dyes involves the following steps: (i) energy of a photon greater than or equal to the band gap energy of the semiconductor is applied and electrons in the valence band are excited to the conduction band leaving the same amount of holes in the valence band, (ii) the photogenerated excitons can be trapped by dissolved oxygen in aqueous solution resulting in the formation of reactive oxygen species (ROS), for instance cOH, and (iii) the ROS can attack and mineralize the adsorbed organic dye molecules. [12][13][14] To date, ZnO and TiO 2 based photocatalysts have been widely studied because of their strong oxidizing power, nontoxic nature, low cost and ease of fabrication and because they are environmentally friendly. [12][13][14][15] But the photocatalytic efficiency of these individual materials remains very low because of the fast recombination of photogenerated excitons in the single phase semiconductor. To overcome this drawback, these semiconductor nanomaterials can be coated, deposited or combined with other metals, semiconductors or carbon based materials. 14, [16][17][18] These nanocomposites can exhibit better and tunable physicochemical properties as compared to those of their counter parts. In the case of the carbon family, graphene has been paid more interest because of its unique optoelectronic properties and many excellent attributes, such as large specic surface area and high transparency. 19,20 Meanwhile, graphene oxide (GO) has been receiving increasing attention because it possesses identical properties to graphene as well as a special surface structure with many hydroxyl and carboxyl groups that help to make various heteronanostructures on its surface. 21 Recent studies have revealed that the governing factors for improving the efficiency of a photocatalyst include increasing the adsorptivity of organic dyes, extending light absorption in the visible range of the solar spectrum and efficient charge separation and transportation of charge carriers to the surface of the photocatalyst, etc. 22,23 Therefore, it is believed that the anchoring of well-organized ZnO NPs on GO nanosheets can effectively utilize the combinative features of ZnO and GO to attain a photocatalyst with superior performance. Junli et al. have synthesized ZnO/graphene oxide nanocomposites and explored their use for the photocatalytic degradation of methyl orange and water splitting. 24 Kamat et al. have studied the interaction between graphene oxide and semiconductors (TiO 2 and ZnO) as well as graphene oxide and metal (Au and Pt) nanoparticles and explored their use for catalysis, energy conversion and fuel cells. 31 Zhang et al. have prepared graphene coated ZnO and explored its use as a photocatalyst for the degradation of methylene blue dye under UV light. They have proposed the Fermi levels as well as the internal electric eld using Kelvin probe force microscopy. 32 Li et al. have synthesized graphene quantum dots modied with ZnO + Cu heterostructures and explored their use for the photocatalytic degradation of rhodamine B under UV light. 33 Tian et al. have synthesized N, S co-doped graphene quantum dot (N, S-GQD)reduced graphene oxide (rGO)-TiO 2 nanotube (TiO 2 NT) composites and explored their use as visible light photocatalysts for the degradation of methyl orange. 34 Tian et al. have fabricated a ternary hybrid of meso-TiO 2 /RGO/CdS and used it as a photocatalyst for the degradation of methylene orange under simulated sunlight. 35 In addition to these reports, various ZnO and graphene based composite photocatalysts were employed for the degradation of various organic dyes as well as the conversion of toxic gases to environmentally friendly products. [36][37][38][39][40][41][42][43] In the present study, a facile, economical and simple chemical approach for the synthesis of FGS/ZnO nanocomposites has been reported. The synthesized FGS/ZnO nanocomposites were explored as photocatalysts for the photodegradation of safranin-T (3,7-diamino-2,8-dimethyl-5-phenyl chloride, C 20 H 19 N 4 Cl, M W ¼ 350.85 g mol À1 ) in an aqueous solution under visible light irradiation. Some of the reported photocatalysts are only useful under UV light which may not be applicable for practical real-life applications, while the synthetic process of some of the other reported photocatalysts is more complicated. Moreover, the proposed synthetic method could be useful for the large scale production of photocatalysts for real life practical applications. In addition, the photodegradation of safranin-T has been explored for the rst time using an FGS/ ZnO photocatalyst and we found excellent photocatalytic activity towards the photodegradation of safranin-T.

Material synthesis
The synthesis of FGS/ZnO nanocomposites involves two steps and they are described as follows.

Synthesis of graphene oxide (GO)
GO was prepared by a well-known modied Hummer's method. 44 About 2 g of graphite powder was added to a 250 mL round bottom ask along with 46 mL of concentrated sulphuric acid. The round bottom ask was kept in an ice bath and about 6 g of potassium permanganate was slowly added into the ask for up to 2 h. Then, the ask was heated to 36 C for 6 h in an oil bath with continuous stirring. Aer that, about 92 mL of deionized water was added dropwise and the stirring continued for a further 15 min. The obtained suspension was transferred into a 5 L beaker and diluted with about 280 mL of water followed by the addition of 5 mL of 30.0% H 2 O 2 . The resulting bright yellow suspension was neutralized (pH ¼ 7) by washing with deionized water several times. Finally, the obtained neutral suspension was centrifuged and the clear suspension was freeze dried for a few days to obtain the GO.
Synthesis of functionalized graphene oxide nanosheet/ZnO nanocomposites (FGS/ZnO NCs) Initially, solution A was prepared by mixing a certain amount of zinc nitrate hexahydrate with ammonium bicarbonate in an aqueous solution, and then 2 mL of aqueous ammonia was added to it. Simultaneously, solution B was prepared by ultrasonication of various amounts of graphene oxide (e.g. 0.05 wt%, 0.09 wt%, 0.10 wt%, 0.50 wt% and 5.00 wt%) in deionized water along with about 0.1 g of PVP. Then, the two solutions were properly mixed and stirred for about 2 h followed by ltration, and washing was carried out with deionized water and ethanol mixture to remove the unbound Zn 2+ ions. The obtained powder samples were dried at 80 C overnight, and then calcined at 300 C for 30 min under air to obtain FGS/ZnO NCs. Similarly, a pristine ZnO NC without GO was also prepared by following the same method without adding the GO as demonstrated above. Photographs of the samples are shown in Fig. S1. †

Characterization of pristine and FGS/ZnO NCs
X-ray diffraction measurements of the pristine ZnO and FGS/ ZnO NCs were carried out using a Rigaku D/max-3B X-ray diffractometer operated at 40 kV and graphite monochromatized Cu K a (l ¼ 1.54Å) was used as the radiation source in a wide-angle region from 20 to 80 on a 2q scale. The morphology of the samples was analysed using a JEOL-1200 Transmission Electron Microscope (TEM) operated at 120 kV. For TEM analysis, a few milligrams of sample were uniformly dispersed in an ethanol solution and a drop of the suspension placed on a carbon coated 150 mesh copper grid and dried naturally under air at room temperature. UV-visible absorption spectroscopy of the FGS/ZnO NC suspension was measured using a UV-visible spectrophotometer (Hitachi, UV-4100) in the range of 300-500 nm. The band gaps of the FGS/ZnO NCs were measured using the same UV-visible spectrometer with BaSO 4 as the reference material. The emission spectra of the FGS/ZnO NCs were recorded using a Hitachi F-4500 uorescence spectrophotometer at an excitation wavelength (l exc ) of 385 nm. The Raman spectra of GO and 0.09 wt% FGS/ZnO NCs were recorded using a Raman microscope (Renishaw) with an excitation energy of l ¼ 514 nm.

Photocatalytic degradation study
For the photocatalytic studies, 100 mL of 2.2 Â 10 À4 M safranin-T aqueous dye solution was prepared in a 250 mL quartz glass beaker. About 20 mg of pristine ZnO and various FGS/ZnO NCs were separately added to the above beaker and stirred for about 1 h in the dark to attain an adsorption equilibrium between the photocatalyst and safranin-T dye. The amount of dye adsorption on the photocatalyst's surface was monitored using a UV-visible spectrometer with a time interval of 20 min. Once it was conrmed that there was no further adsorption of dye on the photocatalyst's surface, the safranin-T dye along with the various photocatalysts contained in the quartz glass beaker was illuminated using a HQ1-400W/D lamp with a 420 nm cut-off lter in the photocatalysis workstation. The distance between the illumination source and the test solution was maintained at about 15 cm. Also, the test quartz beaker was kept under continuous stirring during visible light illumination and water was circulated throughout the photocatalyst chamber to reduce heat generation that could reduce the temperature effect on photocatalytic activity. In addition, a control test was also carried out without adding any photocatalyst. The kinetic study was carried out by using a UV-visible spectrophotometer by withdrawing about a 5 mL aliquot from the test solution with a time interval of about 10 min. The absorbance of the suspension was measured at l max ¼ 518 nm aer separating the dispersed NPs using a centrifuge machine (Cence® TG-16-WS) at 15 000 rpm at room temperature for 5 min. The photocatalytic activity of the FGS/ZnO NC photocatalysts was compared with that of the pristine ZnO NPs as well as with the control. In order to study the role of GO in the adsorption of dye, a blank experiment was also performed where the same concentration of safranin-T dye solution was treated with a maximum GO concentration comprising 5 wt% FGS/ZnO NCs in the absence of visible light illumination. All of the photocatalyst experiments were performed in triplicate and the obtained results are presented as a mean and standard deviation of three analyses.

Measurement of cOH radicals
About 15 mg of pristine ZnO NPs and FGS/ZnO NCs were sonicated for about 10 min in a 3 mM solution of terephthalic acid prepared in a 0.01 M NaOH solution. The reaction mixture was continuously stirred for about 30 min to form adducts between OHc and terephthalic acid. Prior to visible light illumination, emission measurements of the test solution were carried out using a Hitachi F-4500 Fluorescence spectrophotometer at an excitation wavelength (l exi ) of 315 nm. Aer that, the test solution was illuminated under visible light and about a 5 mL aliquot was withdrawn at periodic intervals. Aer centrifugation, the obtained supernatant was examined using the same instrument. A control experiment was also performed without adding the photocatalyst under identical conditions. The total number of OHc radicals generated during the course of the reaction was measured using the uorescence intensity of the adducts formed between OHc and terephthalic acid. 14,45 All of the analyses were performed in triplicate and the results are represented as a mean and standard deviation of three analyses.

Photocatalytic degradation of safranin-T dye in the presence of histidine
We have also studied the role of reactive oxygen species (ROS) towards the photocatalytic degradation of aqueous safranin-T dye solution using histidine as a ROS scavenger. 46,47 About 25 mL test samples comprising the same concentration of safranin-T dye with about 5 mg of 0.09 wt% FGS/ZnO NC and about 45 mg of histidine were continuously stirred under visible light illumination. The time dependent kinetic study of the test solution was carried out using the same UV-visible spectrophotometer. All of the analyses were performed in triplicate and the obtained results are represented as a mean and standard deviation of three analyses.

Results and discussion
Characterization of as-synthesized FGS/ZnO NCs At rst, the phase purity of the pristine ZnO NP and FGS/ZnO (0.09 wt%) NC samples were analysed using XRD analysis and the corresponding results are shown in Fig. 1 48 The crystallite sizes of the ZnO NPs were calculated using the XRD peaks at 2q ¼ 36.3 and they were found to be about 10.3 and 9.3 nm for the pristine ZnO NPs and FGS/ZnO (0.09 wt%) NCs, respectively. However, we haven't observed any diffraction peaks of the functionalized graphene oxide nanosheets, which can be ascribed to the as-synthesized GO nanosheets having either an amorphous nature or a weak crystalline nature. Moreover, the absence of GO diffraction peaks gives indirect evidence for the uniform coverage of ZnO NPs on the surface of FGS and vice versa. To prove the presence of GO in the FGS/ZnO nanocomposites, we have carried out Raman analysis, as shown in Fig. 1b. The Raman spectra of graphene oxide and 0.09 wt% FGS/ZnO nanocomposites show characteristic D and G bands at about 1360 cm À1 and 1605 cm À1 , respectively. The I D /I G ratio was determined to be 1.02 and 1.18 for bare ZnO and 0.09 wt% FGS/ZnO nanocomposites, respectively. These results indicate that there is an increase of defects in the case of 0.09 wt% FGS/ZnO nanocomposites, which can effectively trap the charge carriers and reduce the recombination rate. In addition, one more peak at about 495 cm À1 is observed in the case of 0.09 wt% FGS/ZnO nanocomposites, which could be due to an E 2 high vibration mode associated with the wurtzite type ZnO.
The morphology of the pristine ZnO and FGS/ZnO (0.05 wt%, 0.09 wt% and 5.00 wt%) NCs was examined using TEM analysis and the corresponding gures are shown in Fig. 2. The pristine ZnO NPs show aggregated nanoparticles with an average size of about 10 to 20 nm (Fig. 2a). In the case of FGS/ZnO NCs, strongly adhered ZnO NPs on the surface of FGS have been observed, which can be ascribed to strong bonding between the ZnO NPs and the functionalized surface of the GO nanosheets. In the case of the FGS/ZnO NCs, 0.05 wt% FGS supported ZnO shows a slight aggregation of ZnO NPs on the surface of FGS (Fig. 2b), while 0.09 wt% FGS supported ZnO shows better deposition of ZnO NPs with uniform distribution observed (Fig. 2c). 5.00 wt% FGS supported ZnO shows more free space with a lesser amount of ZnO NPs on the surface of FGS (Fig. 2d). Fig. 2e clearly shows lattice spacing of about 0.33 nm and 0.28 nm due to the (002) plane of graphene and (100) plane of ZnO, respectively. The close lattice spacing between ZnO and FGS can favour fast carrier transfer and separation. The EDS spectrum conrms the presence of zinc, oxygen and carbon in 0.09 wt% FGS/ZnO nanocomposites and also indicates the uniform distribution of all of the elements in the 0.09 wt% FGS/ZnO nanocomposite (Fig. 2f). These results give strong evidence for the formation of FGS/ZnO nanocomposites. These results suggest that 0.09 wt% FGS supported ZnO can be a better photocatalyst for the degradation of dye due to the uniform distribution of ZnO NPs that can efficiently absorb the visible light and effectively separate the charge carriers at the surface of a photocatalyst. Moreover, the disappearance of wrinkles of FGS is observed, which can be ascribed to the uniform decoration of ZnO NPs on exfoliated functionalized GO nanosheets.

Optical studies of as-synthesized FGS/ZnO NCs
The optical properties of pristine ZnO NPs and various compositions of FGS/ZnO NCs were studied using UV-visible spectroscopy and photoluminescence spectroscopy. Initially, the optical band gaps of the samples were studied using UVvisible diffuse reectance spectroscopy and the corresponding gures are shown in Fig. 3a and b. The pristine ZnO NPs and various FGS/ZnO NCs showed absorption between 390-420 nm. The band gaps of the samples were measured using Tauc plots (Fig. 3b). 49 The pristine ZnO NPs showed a band gap of about 3.16 eV, which is blue shied to that of bulk ZnO (about 3.38 eV), which can be attributed to the smaller size of the ZnO NPs as well as quantum connement. 50,51 The FGS/ZnO NCs exhibited band gaps of about 3.13, 3.10, 3.12, 3.18 and 3.27 eV corresponding to 0.05 wt%, 0.09 wt%, 0.10 wt%, 0.50 wt% and 5.00 wt% of the FGS/ZnO NCs, respectively. Among the FGS/ZnO NCs, 0.09 wt% FGS/ZnO NCs exhibited a lower band gap and a blue shi of about 0.06 eV as compared to those of pristine ZnO NPs, which can be attributed to the quantum connement of ZnO NPs on the surface of FGS. 50,51 In addition, the increased absorbance of the FGS/ZnO NCs (0.05 wt%, 0.09 wt% and 0.10 wt%) in the visible region as compared to that of pristine ZnO indicates the formation of visible light photocatalysts and that they can be effective for practical photocatalytic applications under visible light or sunlight. These band gap results further supported the higher photocatalytic activity of 0.09 wt% FGS/ZnO NCs in visible light.
The photoluminescence spectra of pristine ZnO NPs and various FGS/ZnO NCs are shown in Fig. 4. The PL spectra of pristine ZnO NPs as well as FGS/ZnO NCs show weak emission bands at 435 nm, 466 nm and 485 nm. The emission band in the blue region at 435 nm is ascribed to the electronic transition between interstitial oxygen (O i ) and the excitonic level. 18,52 Another emission in the blue-green region of about 466 nm is ascribed to the electronic transition between a shallow donor (Zn i ) and deep acceptor (V Zn ). 14,53 The PL emission in the green region of about 485 nm is attributed to interstitial zinc, structural defects and zinc vacancies. 53 In addition, 0.50 wt% and 5.00 wt% FGS/ZnO NCs exhibit a strong new green emission at about 565 nm ascribed to structural defects caused by oxygen vacancies. 25 The green emission peak intensity is increased by increasing the concentration of FGS indicating that there are more structural defects that reduce the photocatalytic activity of the high loaded FGS NCs. Additionally, a decrease in PL emission intensity is observed for 0.09 wt% FGS/ZnO NCs compared

Photocatalytic studies
Before visible light illumination on the test solution, we have examined the effect of FGS concentration in FGS/ZnO NCs on adsorption. According to literature, the available functional groups such as hydroxyl, carbonyl and epoxy groups on the surface of the GO nanosheets, and the p-p conjugation and 2-D planar structure can contribute to the adsorption of dye molecules on its surface. 24,25 To study the adsorption of dye on the surface of FGS/ZnO NCs, 20 mg of various photocatalysts were dispersed into 100 mL of 2.2 Â 10 À4 M dye solution and stirred for about 7 h under dark conditions. Interestingly, almost complete adsorption of safranin-T dye onto the surface of the 5.00 wt% FGS/ZnO NCs was observed as compared that adsorbed by the 0.09 wt% sample, which could be due to the availability of a higher amount of surface functional groups on the surface of FGS for dye adsorption (Fig. S2 †). 24,25 In this way, the role of FGS on the adsorption of safranin-T dye in the FGS/ZnO NCs was established. Next, the photocatalytic activity of the pristine ZnO NPs and FGS/ZnO NCs was examined towards the photodegradation of safranin-T dye in an aqueous solution under visible light and the corresponding results are shown in Fig. 5. The observed results indicate that FGS/ZnO NCs (0.05 wt%, 0.09 wt% and 0.10 wt%) possess higher photodegradation efficiency than the pristine ZnO NPs, FGS/ZnO NCs (0.50 wt% and 5.00 wt%) and control sample (Fig. 5a). The lower photocatalytic activity of 0.50 wt% and 5.00 wt% FGS/ZnO NCs than that of other FGS/ZnO NCs could be due to a shielding effect. By increasing the concentration of FGS in FGS/ZnO NCs, they are able to shield the active sites on the surface of the photocatalyst and signicantly reduce the penetration of light to the active centres. 27 In addition, the higher concentration of FGS leads to more opacity and light scattering results that show a decrease in the intensity of light penetration to the active centres of the photocatalyst. 26 Moreover, the increased concentration of FGS in FGS/ZnO NCs can absorb some of the light and cause the problem of light harvesting competition between the counter parts of the FGS/ZnO NC. 2 This leads to high recombination centres instead of providing an efficient electron pathway and thus reduces the photocatalytic activity.
Kinetic studies were performed for all of the samples and the corresponding results are given in Fig. 5b and c. The photodegradation of safranin-T dye follows pseudo-rst-order kinetics, which can be written as 14 where C o and C t are the concentrations of safranin-T dye at time ¼ 0 and time ¼ t, respectively, and k is the apparent pseudo-rst-order rate constant. The linear relationship between ln(C o /C t ) and irradiation time indicates that the photodegradation of safranin-T dye follows pseudo-rst-order kinetics. 18 The apparent pseudo-rst-order rate constant (k) was calculated from the slope of the plot of ln(C o /C t ) vs. time 't'. The estimated apparent pseudo-rst-order rate constant (k) values for the degradation of safranin-T are 0.018, 0.026, 0.049, 0.031, 0.017 and 0.014 min À1 for pristine ZnO, and 0.05 wt%,  0.09 wt%, 0.10 wt%, 0.50 wt% and 5.00 wt% FGS in FGS/ZnO NCs, respectively. The order of photodegradation efficiency of the photocatalysts is 0.09 wt% FGS/ZnO NCs > 0.10 wt% FGS/ ZnO NCs > 0.05 wt% FGS/ZnO NCs > pristine ZnO > 0.50 wt% FGS/ZnO NCs > 5.00 wt% FGS/ZnO NCs (Fig. 5d). The higher degradation efficiency of 0.09 wt% FGS/ZnO NCs as compared to that of pristine ZnO and other FGS/ZnO NCs could be due to the effective separation of charge carriers as well as the effective transportation of charge carriers to the surface of the photocatalyst, which can be seen in the PL spectra of the FGS/ZnO NCs in Fig. 4. The decreased photocatalytic activity in the cases of 0.50 wt% and 5.00 wt% FGS/ZnO NCs could be due to the formation of a higher amount of oxygen vacancies, which is evident from the intense emission band at 565 nm (Fig. 4). The observed results corroborate well with the reported literature on the photocatalytic degradation of various dyes using ZnO/rGO nanocomposites. 27 The photodegradation efficiency of various ZnO/graphene or ZnO/graphene oxide composite photocatalysts are summarized and shown in Table S1. † The reusability of a photocatalyst elucidates its stability and activity. One of the important problems associated with using ZnO NPs as a photocatalyst is that they have lower photostability and can easily undergo photoinduced dissolution. 55 The possible photocorrosion reaction can be expressed as follows: The most probable reason for photocorrosion of ZnO is due to the reaction of holes present in the valence band with surface oxygen at the solid interface of the photocatalyst. To test the photocatalytic stability (reusability) 0.09 wt% FGS/ZnO NCs and pristine ZnO were chosen and photocatalytic experiments were carried out for up to 5 cycles (Fig. S3 †). The 0.09 wt% FGS/ZnO NCs showed about 4% lower degradation aer ve cycles while the activity of pristine ZnO was drastically reduced, indicating good stability and durability of the 0.09 wt% FGS/ZnO NCs over pristine ZnO NPs. These results demonstrate that the combination of optimized FGS and ZnO improves the photostability as well as the photocatalytic activity of the FGS/ZnO NCs.
The proposed possible mechanism for the photodegradation of safranin-T by FGS/ZnO NCs is shown in Fig. 6. 24,27,29 Upon visible light illumination, electrons (e À ) present in the valence band of ZnO are excited to the conduction band and leave the same number of photogenerated holes (h + ) in the valence band. Then, the electrons present in the conduction band of ZnO are able to transfer to the functionalized GO nanosheets due to strong interfacial contact between ZnO and FGS, which effectively hinders the recombination rate of photoexcited excitons and effectively transports the charge carriers towards the surface of the photocatalyst. The offset face-to-face free safranin-T dye adsorbed over the surface of FGS via p-p interactions can be directly oxidized by the holes present in the valence band of ZnO. In addition, the electrons present on the surface of the photocatalyst are readily trapped by dissolved oxygen (O 2 ) in the aqueous solution and produce superoxide radical anions (O 2 c À ). The reactive active species such as holes (h + ), superoxide radical anions (O 2 c À ) and hydroxyl radicals (cOH) are responsible for the mineralization of safranin-T dye into various eco-friendly intermediates. 24,27 In the present case, the real VB and CB of ZnO in FGS/ZnO and bare ZnO have been estimated theoretically according to Mulliken electronegativity theory. 45 here, E VB , E CB and E g correspond to the valence band, conduction band and band gap of the individual semiconductor. X is the absolute electronegativity of the corresponding semiconductor. The VB and CB of bare ZnO and various FGS/ZnO NCs were calculated and presented in Table S2. † The observed VB and CB band positions indicate that 0.09 wt% FGS/ZnO NCs possess a lower conduction band and lower valence band than other FGS/ZnO NCs as well as bare ZnO, which facilitates fast electron transport to the surface and enhances photocatalytic activity towards the photodegradation of safranin-T dye. The increased photocatalytic activity of FGS/ZnO NCs could be due to the following factors: 27 (i) the enhanced safranin-T dye adsorption on the surface of FGS via p-p interactions which could be due to the optimum amount of FGS in the FGS/ZnO NCs (Fig. S2 †), and (ii) FGS being able to act as an efficient support for the strong adherence of ZnO NPs, this combination can help effective separation of the photogenerated excitons as well as effective transportation of the charge carriers towards the surface of the photocatalyst for efficient mineralization of the safranin-T dye (Fig. 4).
ZnO NPs are known to produce reactive oxygen species (ROS) by interacting with aqueous media. 46 In the present study, the generation of hydroxyl radicals over the surface of the photocatalysts during the photocatalytic study was conrmed using Fig. 6 Proposed photocatalytic mechanism for the degradation of safranin-T dye using FGS/ZnO NCs. 24,27,29 terephthalic acid as a probe molecule. 45,56 The intensity of the PL emission was monitored at a l max of 425 nm corresponding to the formation of the adduct i.e. 2-hydroxy terephthalic acid (TAOH) formed via the reaction between terephthalic acid and OHc generated during the interaction of pristine ZnO and FGS/ ZnO NCs in safranin-T dye solution (Fig. 7a).
The order of PL emission peak intensity was found to be 0.09 wt% FGS/ZnO NCs > 0.10 wt% FGS/ZnO NCs > 0.05 wt% FGS/ZnO NCs > pristine ZnO > 0.50 wt% FGS/ZnO NCs > 5.00 wt% FGS/ZnO NCs. The observed order coincides with the PL intensities of pristine ZnO and FGS/ZnO NCs (Fig. 4). The observed results indicate that the 0.09 wt% FGS/ZnO NCs can produce a higher amount of OHc than other photocatalysts, which supports the higher photocatalytic activity of 0.09 wt% FGS/ZnO NCs compared to that of other photocatalysts. 45,56 In order to determine the role of ROS generation towards the photodegradation of safranin-T dye, we have designed an experiment to scavenge the generated ROS during the photodegradation of safranin-T dye in an aqueous solution. Here, histidine was used as the scavenger, which is a well-known scavenging agent for OHc and singlet oxygen. 46,47 Prior to the use of histidine as a scavenger, we carried out a control experiment with 45 mg of histidine and without any photocatalyst using visible light illumination to study the effect of histidine on the photodegradation of safranin-T. The observed results indicate negligible photodegradation of safranin-T dye by histidine (Fig. 7b). Aer that, the same amount of histidine was introduced along with 20 mg of 0.09 wt% FGS/ZnO NC photocatalyst in 100 mL of safranin-T dye solution with visible light illumination and the photodegradation of safranin-T dye was monitored using UV-visible spectroscopy. The photodegradation of safranin-T dye was strongly inhibited (about 20% photodegradation of safranin-T dye), indicating that histidine strongly scavenges the generated OHc during photocatalysis. The observed results strongly support the idea that photodegradation of safranin-T dye was induced by ROS generated during photocatalysis. 46,47 Conclusion FGS/ZnO NCs with enhanced photocatalytic activity towards the photodegradation of safranin-T dye in aqueous solution have been successfully synthesized via an economical, facile and simple solution route followed by calcination under environmental conditions. The effect of FGS on dye adsorption as well as photodegradation was explored. The photocatalyst with 0.09 wt% FGS/ZnO NCs exhibits high photocatalytic activity compared to pristine ZnO as well as other FGS/ZnO NCs. The enhancement in photodegradation of safranin-T dye with 0.09 wt% FGS/ZnO NC photocatalyst was attributed to the fact it had an optimum amount of FGS for effective adsorption of safranin-T dye on the surface of FGS as well as an effective separation of charge carriers for the mineralization of safranin-T dye. The increased amount of FGS causes more oxygen defects on the surface of the photocatalyst, which causes reduced activity by the shielding effect phenomenon. The role of ROS generation during the photocatalytic degradation of safranin-T dye was veried by PL measurement that used terephthalic acid as a probe molecule as well as a scavenger test by histidine. The reported synthetic method can be extended to prepare other FGS/semiconductor NCs for various functional applications.

Conflicts of interest
There are no conicts to declare.