Efficient MoWO3/VO2/MoS2/Si UV Schottky photodetectors; MoS2 optimization and monoclinic VO2 surface modifications
Mohamed A. Basyooni, Shrouk E. Zaki, Mohamed Shaban, Yasin Ramazan Eker, Mücahit Yılmaz
Abstract
Abstract The distinctive properties of strongly correlated oxides provide a variety of possibilities for modulating the properties of 2D transition metal dichalcogenides semiconductors; which represent a new class of superior optical and optoelectronic interfacing semiconductors. We report a novel approach to scaling-up molybdenum disulfide (MoS 2 ) by combining the techniques of chemical and physical vapor deposition (CVD and PVD) and interfacing with a thin layer of monoclinic VO 2 . MoWO 3 /VO 2 /MoS 2 photodetectors were manufactured at different sputtering times by depositing molybdenum oxide layers using a PVD technique on p-type silicon substrates followed by a sulphurization process in the CVD chamber. The high quality and the excellent structural and absorption properties of MoWO 3 /VO 2 /MoS 2 /Si with MoS 2 deposited for 60 s enables its use as an efficient UV photodetector. The electronically coupled monoclinic VO 2 layer on MoS 2 /Si causes a redshift and intensive MoS 2 Raman peaks. Interestingly, the incorporation of VO 2 dramatically changes the ratio between A-exciton (ground state exciton) and trion photoluminescence intensities of VO 2 /(30 s)MoS 2 /Si from < 1 to > 1. By increasing the deposition time of MoS 2 from 60 to 180 s, the relative intensity of the B-exciton/A-exciton increases, whereas the lowest ratio at deposition time of 60 s refers to the high quality and low defect densities of the VO 2 /(60 s)MoS 2 /Si structure. Both the VO 2 /(60 s)MoS 2 /Si trion and A-exciton peaks have higher intensities compared with (60 s) MoS 2 /Si structure. The MoWO 3 /VO 2 /(60 s)MoS 2 /Si photodetector displays the highest photocurrent gain of 1.6, 4.32 × 10 8 Jones detectivity, and ~ 1.0 × 10 10 quantum efficiency at 365 nm. Moreover, the surface roughness and grains mapping are studied and a low semiconducting-metallic phase transition is observed at ~ 40 °C.