2017
DOI: 10.1088/1757-899x/202/1/012042
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Crystal Structure, Optical, and Electrical Properties of SnSe and SnS Semiconductor Thin Films Prepared by Vacuum Evaporation Techniques for Solar Cell Applications

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Cited by 9 publications
(4 citation statements)
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“…The value of the lattice constant for the different materials has been taken from previous research. The lattice mismatch of MoS 2 and In 2 Te 3 is 8.69%, which is lower than that of the HTLs employed in the previous studies. The primary cause of non-radiative recombination is the presence of defect and interface defect density, which results in carrier losses and a drop in output voltage .…”
Section: Resultsmentioning
confidence: 99%
“…The value of the lattice constant for the different materials has been taken from previous research. The lattice mismatch of MoS 2 and In 2 Te 3 is 8.69%, which is lower than that of the HTLs employed in the previous studies. The primary cause of non-radiative recombination is the presence of defect and interface defect density, which results in carrier losses and a drop in output voltage .…”
Section: Resultsmentioning
confidence: 99%
“…The peaks corresponding to Sn 3d 3/2 at 487.6 eV and Sn 3d 5/2 at 496.1 eV are singlets for Sn. , For Se, binding energy peaks at 55.8 and 54.4 eV correspond to Se 3d 3/2 and Se 3d 5/2 states, respectively. These binding energy values for 3d electronic states of Sn and Se correspond to SnSe stoichiometry. Figure S1a–d (Supporting Information) shows the crystal structures of SnSe at room temperature with the Pnma space group along the a , b , and c axis; here, gray balls indicate Sn atoms; yellow balls indicate Se atoms. The box outlines a single unit cell with eight atoms …”
Section: Results and Discussionmentioning
confidence: 99%
“…Given that no surfactant has been used, the shape and growth mechanism of the SnSe flakes are primarily determined by the anisotropic crystal structure of SnSe. SnSe crystallizes in an orthorhombic unit cell with lattice parameters a = 11.47 Å, b = 4.152 Å, and c = 4.439 Å, in a layered structure having strong covalent intralayer bonding and weak van der Waals interlayer bonding (Figure a). , The layers are perpendicular to the longest axis ( a -axis), hence, only weak van der Waals forces exist along this direction. When thermally decomposed Se and Sn atoms reach the substrate at elevated temperatures, the nucleation centers first form on the substrate’s physically or chemically heterogeneous sites (often on the substrate’s defect sites).…”
Section: Resultsmentioning
confidence: 99%