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Department, University, Abstract Results and Discussion Topic Name* Department, University, E-mail: Introduction References Conclusions Experimental Procedure logo logo   Development of heterostructured semiconductor photocatalyst makes a significant advancement in catalytic technologies. Highly crystalline Bi2S3−ZnO nanosheets with hierarchical structure has been successfully synthesized by a facile sonochemical process and characterized by X−ray diffraction (XRD), High Resolution Scanning Electron Microscopy (HR−SEM), X-ray photoelectron spectroscopy (XPS), UV−Vis diffuse reflectance spectroscopy (DRS), Photoluminescence spectroscopy (PL) and Brunauer−Emmett−Teller (BET) surface area measurements. X-Ray powder diffraction (XRD) analysis reveals that the as synthesized product has orthorhombic phase of Bi2S3 and hexagonal wurtzite phase of ZnO. The XPS analysis shows the presence of Zn, O, Bi and S elements and their oxidation states. Bi2S3−ZnO has increased absorption in the UV as well as visible region. This heterostructured nano catalyst shows higher photocatalytic activity for the degradation of Acid Black1 (AB 1) under UV−A light than pure ZnO, Bi2S3 and commercial Degussa P25. The heterojunction in Bi2S3−ZnO photocataslyst led to the low recombination rates of photoinduced electron−hole pairs and enhanced photocatalytic activity. Bi2S3−ZnO is more advantageous in AB 1 degradation because of its reusability and higher efficiency at the neutral pH 7. Environmental Water pollution is one of the biggest problems that we face today. It is a global crisis that needs people in every country to work together, protecting our environment and improving before it’s too late Use of non-toxic photocatalyst for removal of toxic dyes Field Emission Scanning Electron Microscopy Binding Energy (eV) 800 1000 600 400 200 (a) Intensity (x 103 counts/s) Zn 3d Zn 3p L2 M 45 M 4 5 O 1s L3 M 45 M 4 5 O KVV Zn 2p3/2 Zn 2p1/2 Bi 5d5 Bi 4f 7/2 Bi 4f 5/2 C 1s Bi 4d 30 60 90 12 0 S 2p S 2s Intensity (x 102 counts/s) S 2p1/2 164.2 162.1 S 2p3/2 166 164 162 160 158 (e) 15 45 164.1 158.6 Bi 4f5/2 Bi 4f7/2 172 168 156 152 Bi 4f (d) 174 50 100 150 1056 1048 1040 1032 1024 1016 Zn 2p 1045.1 1021.9 (c) 1064 40 80 120 Intensity (x 103 counts/s) 532.8 O-H O-L 548 544 540 536 532 528 524 (b) 530.8 20 X-ray photoelectron spectroscopy Diffuse Reflectance Spectra X-ray diffraction studies High-Resolution Scanning Electron Microscopy Bi2S3−ZnO shows many fold increased absorption in the ultraviolet region of 200-400 nm indicating more photocatalytic activity in UV. There is a slight increase in absorbance in visible region. (a) prepared ZnO and (b) Bi2S3-ZnO Photoluminescence Spectra Catalysts show a near UV emission band at 416 nm and a blue–green band at 485 nm. This near UV emission corresponds to the exciton recombination related near−band edge emission of ZnO. Reduction of PL intensity at 416 nm for Bi2S3−ZnO when compared to prepared ZnO and Bi2S3 indicates the suppression of recombination of the photogenerated electron–hole pair by Bi2S3 loaded on ZnO. This leads to a higher photocatalytic activity. (a) Bi2S3 , (b) prepared ZnO and (c) Bi2S3-ZnO All peaks of Bi2S3 and ZnO absolutely matched with Bi2S3−ZnO (Fig. c). XRD pattern of Bi2S3−ZnO reveals the presence of orthorhombic form of Bi2S3 in hexagonal wurtzite ZnO base material These images show that Bi2S3−ZnO is a mixture of nano sheets and nano particles The enlarged images confirm the heteroarchitectured form of the catalyst containing nanosheets and nanoparticles. The nanosheets have a breath of 34.2 nm with the length in the range of 240.9 to 656.8 nm (Fig. 2a). O1s profile is asymmetric and can be fitted to two symmetrical peaks α and β locating at 530.8 and 532.8 eV, respectively, indicating two different kinds of O species in the sample (Fig. b). The peaks α and β should be associated with the lattice oxygen (OL) of ZnO and chemisorbed oxygen (OH) caused by the surface hydroxyl, respectively. Fig. c presents the XPS spectra of Zn 2p, and the peak positions of Zn 2p1/2 and Zn 2p3/2 locate at 1045.1 eV and 1021.9 eV. we can conclude that Zn is in the state of Zn2+. The signals of Bi 4f7/2 and Bi 4f5/2 at 158.6 and 164.1 eV (Fig. d), reveal that Bismuth is in the state of Bi3+. Two signals of S 2p1/2 and S 2p3/2 at binding energies of 164.2 and 162.1eV indicate the presence of sulfide species S2- (Fig. e). FESEM images shows a mixture of nanosheets and nano particles. The nanosheets attached with another nanosheet and form inter cross sectioned walls. The nanosheets were made up of Bi2S3 as confirmed by EDS analysis. The nanoparticles were made up of ZnO. The nanoparticles have uniform structure and large number of cavities in the surface of Bi2S3-ZnO. These cavities favour the adsorption of dye molecules in the surfaces of the heteroarchitectured material. (a) prepared ZnO and (b) Bi2S3-ZnO Photocatalytic activity Effect of pH Reusability of the catalyst After 90 min of irradiation the percentages of AB 1 degradation are 46, 73, 96, 63 and 32% at pH 3, 5, 7, 9 and 11, respectively. To find out the reason for the effect of pH on degradation efficiency, zero point charge (ZPC) of the catalyst was determined by potentiometric titration method. Zero point charge of Bi2S3-ZnO was found to be 7.3, which is less than ZPC of ZnO (9). When the pH is above ZPC, the surface charge density of the catalyst becomes negative. This decreases the adsorption of dye molecules, which exist anionic at pH above 7. Hence the degradation efficiency is low at pH 9 and 11. Dye is resistant to self photolysis. Under dark condition there is a decrease of dye concentration initially with Bi2S3−ZnO and this is due to adsorption of dye on the catalyst. Under UV−light irradiation, degradation of AB 1 occurred with all the catalysts. Almost complete degradation (96.0%) of dye was attained in 90 min with Bi2S3−ZnO and UV light. Percentages of degradation with ZnO, Bi2S3 and TiO2−P25 were 76.1, 69.1 and 59 respectively for 90 min irradiation. AB 1 dye with Bi2S3−ZnO under different irradiation times Bi2S3−ZnO exhibits remarkable photostability as the AB 1 degradation percentages are 96.0%, 95%, 93%, 93% and 93% in the first, second, third, fourth and fifth runs respectively for 90 min. There is no significant change in the degradation efficiency of Bi2S3−ZnO after 3rd cycle. -0.2 -0.1 0.0 +1.0 +2.0 +3.0 +4.0 Energy (eV) Vs NHE (eV) ZnO Bi2S3 h+ h+ h+ h+ h+ h+ h+ e- e- e- e- e- e- e- VB CB O2 O.- + Organic Dye H2O + CO2 + Mineral acids H2O OH Dark 30min 45min 60min 90min e- h+ Dark 30 min 45 min 60 min 90 min % of AB 1 remaining Time (min) Bi2S3−ZnO semiconductor photocatalyst was synthesized by a simple and cost effective sonochemical method and characterized. XRD and XPS reveal the presence of Zn, O, Bi and S and their oxidation states in the catalyst. HR−SEM images show a mixed of nano sheets and nanoflower like hierarchical structure of Bi2S3−ZnO. Bi2S3−ZnO has many fold increase in UV absorption when compared to ZnO. The excellent photocatalytic activity stems from the different conduction band edge positions of Bi2S3 and ZnO, which promote electron transfer from Bi2S3 to ZnO and holes transfer from ZnO to Bi2S3 reducing electron-hole recombination. This heterojunction photocatalyst exhibits much enhanced photocatalytic activity in degradation of Acid Black 1 under UV light. Bi2S3−ZnO was found to be stable and reusable without appreciable loss of catalytic activity up to five runs. As this heterostructured catalyst is reusable with maximum efficiency at neutral pH 7 it will be very useful as industrial catalyst for effective treatment of dye effluents. 1 A. McLaren, T. Valdes Solis, G. Li and S. C. Tsang, J. Am. Chem. Soc., 2009, 131, 12540. 2 N. Kislov, J. Lahiri, H. Verma, D. Y. Goswami, E. Stefanakos and M. Batzill, Langmuir, 2009, 25, 3310. 3 M. D. Hernandez Alonso, F. Fresno, S. Sareza and J. M. Coronado, Energy Environ. Sci., 2009, 2, 1231. 4 D. Yiamsawas, K. Boonpavanitchakul and W. Kangwansupamonkon, J. Microscopy. Soc.Thailand, 2009, 23, 75. 5J. F. Moudler, W. F. Stickle, P. E. Sobol and K. D. Bomben, Handbook of X-ray Photoelectron Spectroscopy Perkin-Elmer: Eden Prairie, MN, 1992. 6 C. D. Wagner, W. M. Riggs, L. E. Davis and J. F. Moulder, Handbook of X-ray Photoelectron Spectroscopy, Perkin Elmer: Eden Prairie, 1979, 81. 7 Y. Schuhl, H. Baussart, R. Delobel, M. Le Bras, J. Leroy, L. G. Gengembre and Rimblot, J. Chem. Soc. Faraday Trans., 1983, 79, 2055. 8 S. Subramanian, J. S. Noh and J. A. Schwarz, J. Catal., 1988, 114, 433. 9 R. Velmurugan, B. Krishnakumar, B. Subash and M. Swaminathan, Sol. Energy Mater. Sol. Cells, 2013, 108, 205-212. 10 D. K. Ma, M. L. Guan, S. S. Liu, Y. Q. Zhang, C. W. Zhang, Y. X. He and S. M. Huang, Dalton Trans., 2012, 41, 5581.