First-principles study of the sulfur K and L2,3 edges of transition metal disulfide monolayers,MS2 (M=Mo,W and Re) |
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Affiliation: | 1. Department of Solid Mechanics and Design, Faculty of Mechanical Engineering, University Technology Malaysia – UTM, 81310 UTM Skudai, Johor, Malaysia;2. School of Engineering, Griffith University, Gold Coast Campus, Southport 4222, Australia;3. School of Engineering, The University of Newcastle, Callaghan, New South Wales 2308, Australia;1. Department of Physics, University of Mohaghegh Ardabili, P.O. Box 179, Ardabil, Iran;2. Department of Physics, Science and Research Branch, Islamic Azad University, Tehran, Iran;3. Department of Physics, Babol Noshirvani University of Technology, Shariati Ave., Babol, 47148-71167, Iran;1. Graphic Era University, Bell Road, Clement Town, Dehradun, India;2. Department of Electronic Science, University of Delhi South Campus, Benito Juarez Road, New Delhi 110021, India;3. School of Materials Science and Engineering, Gwangju Institute of Science Technology (GIST), Gwangju 500-712, Republic of Korea;4. Department of Physics, Gurukula Kangri University, Haridwar 249404, India;5. National Physical laboratory (NPL), New Delhi, India;6. School of Engineering & Technology, Sharda University, Greater Noida 201306, India |
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Abstract: | By means of the energy loss near edge structure (ELNES) analysis, the electronic structures of layered transition metal disulfides were studied. In the framework of full potential linearized augmented plane wave method, ELNES spectra of sulfur K and L2,3 edges of layered MoS2, WS2 and ReS2 have been calculated at magic angle conditions, and compared with those of bulks and the only existing experimental fine structure. Compared to the bulks, the energy differences between the main peaks in sulfur K and L2,3 edges of monolayers decrease due to the slightly larger bond lengths that it can be used as a fingerprint for monolayers. Sulfur K edges in monolayers include some main features originated from electron transition to pz (π) and px+py (σ) states and their hybridization. The overall dispersions of the sulfur L2,3 edges in all cases are similar to the d-symmetry density of states. The first two features in L2,3 edge of bulks and monolayers can be attributed to electron transition of sulfur 2p to the both unoccupied 3s-like states of sulfur and 4d states of transition metal atoms. Due to the considerable amount of s states at the energy position of a shoulder like structure in L2,3 edge of both bulks and monolayers, these structures can be assigned to the sulfur 2p electron transition to unoccupied sulfur 3s states. The other features at higher energies are due to the transition of sulfur 2p electrons to the d-symmetry states of sulfur. In addition, due to the considerable energy band gaps, it seems that the use of core–hole approximation is essential for accurate reproduction of ELNES features of transition metal disulfides. |
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Keywords: | Transition metal disulfides Monolayers ELNES Sulfur K and L2,3 edges Core–hole approximation |
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