| Autor: |
Alex KV; Department of Physics, School of Basic and Applied Sciences , Central University of Tamil Nadu , Thiruvarur 610 005 , India., Prabhakaran A; Department of Physics, School of Basic and Applied Sciences , Central University of Tamil Nadu , Thiruvarur 610 005 , India., Jayakrishnan AR; Department of Physics, School of Basic and Applied Sciences , Central University of Tamil Nadu , Thiruvarur 610 005 , India., Kamakshi K; Department of Physics , Madanapalle Institute of Technology & Science , Madanapalle 517325 , Andhra Pradesh , India., Silva JPB; Centro de Fısica das Universidades do Minho e do Porto (CF-UM-UP) , Campus de Gualtar , Braga 4710 057 , Portugal., Sekhar KC; Department of Physics, School of Basic and Applied Sciences , Central University of Tamil Nadu , Thiruvarur 610 005 , India. |
| Abstrakt: |
In this work, we proposed an efficient heterostructure photocatalyst by integrating the ferroelectric BaTiO 3 (BTO) layer with the semiconductor MoO 3 layer, availing the ferroelectric polarization of BaTiO 3 and high generation of photoinduced charge carriers in the MoO 3 layer. The effect of MoO 3 layer thickness ( t MoO 3 ) on the photocatalytic efficiency of the BTO/MoO 3 heterostructures is found to be optimum at t MoO 3 = 67 nm as t MoO 3 varies from 40 to 800 nm. The BTO/MoO 3 heterostructure with t MoO 3 = 67 nm exhibits a high efficiency of 86% for the degradation of rhodamine B (RhB) under the exposure of UV-visible light for 60 min. The photocatalysis rate kinetics analysis reveals that the rate constant in the heterostructure is 1.7 times of pure BTO and 3.2 times of pure MoO 3 films. The enhanced photocatalytic activity in the heterostructures is attributed to the electric field-driven carrier separation due to the ferroelectric polarization and the heterojunction band bending. The charge coupling effect between BaTiO 3 and MoO 3 is evident from the current-voltage characteristics. The maximum lattice strain in the heterostructure with t MoO 3 = 67 nm as evident from X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR), and photoluminescence (PL) analysis further confirms the charge transfer between the layers. The degradation as well as decolorization efficiency of the BTO/MoO 3 heterostructure is higher than that of pure BTO and MoO 3 films. Radical trapping experiments reveal that electrons are the major contributors to the photocatalytic activity of the BTO/MoO 3 heterostructure. The reusability test shows only a reduction of 5% in the efficiency of the heterostructure after five photocatalysis cycles. The heterostructure can also efficiently decompose the other dyes such as rose bengal and methyl violet. Thus, our findings prove that an efficient and reusable photocatalyst can be designed through the integration of the ferroelectrics with the semiconductor layers. |
