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Publication highlights

1.
Guido Roma, Elaheh Ghorbani, Hossein Mirhosseini, Janos Kiss, Thomas D. Kühne, and Claudia Felser, "Predicting the stability of surface phases of molybdenum selenides," Applied Physics Letters 104 (6), 1-4 (2014).
2.
Hossein Mirhosseini, Guido Roma, Janos Kiss, and Claudia Felser, "First-principles investigation of the bulk and low-index surfaces of MoSe2," Physical Review B 89 (20), 1-8 (2014).

Large scale ab-initio calculations

In the framework of the ComCIGS-II project our team performs large scale ab-initio calculations on the materials related to thin film solar cells, focusing on three main areas of interest:

  • the properties of the light absorber layer involving materials like CuInSe2, CuInS2, CuGaSe2, CuIn5Se8, (see Figure 1) and their interaction with various impurities from the buffer layer (CdS, Zn(O,S)), and the effect of Na and K dopants on the atomic and electronic structure of these materials
<div style="text-align: justify;"><strong>Figure 1:</strong> Conventional tetragonal unit cell of CuInSe<sub>2</sub> (left). The tetragonal chalcopyrite-like CuIn<sub>5</sub>Se<sub>8</sub> ordered vacancy compound (right) can be structurally understood as taking a &radic;2 x&nbsp;&radic;2 x 1&nbsp;supercell of CuInSe<sub>2 </sub>(show in the center), and substituting two Cu atoms with In (denoted as In<sub>Cu</sub>), and four Cu atoms are removed, leading to four pristine Cu-vacancy sites denoted as V<sub>Cu</sub>.</div> Zoom Image
Figure 1: Conventional tetragonal unit cell of CuInSe2 (left). The tetragonal chalcopyrite-like CuIn5Se8 ordered vacancy compound (right) can be structurally understood as taking a √2 x √2 x 1 supercell of CuInSe2 (show in the center), and substituting two Cu atoms with In (denoted as InCu), and four Cu atoms are removed, leading to four pristine Cu-vacancy sites denoted as VCu.
  • the chemisorption, diffusion and reaction of Se, Na, K and O on the Mo surfaces, adsorbate patterns, and simulating scanning tunnelling microscopy (STM) images to provide guidelines for future experiments (see Figure 2)
<div style="text-align: justify;"><strong>Figure 2:</strong> The left panel shows the stability ranges for the most stable adsorption patterns/coverages of Se on the Mo(110) surface in equilibrium with a gas of Se2 molecules. The patterns corresponding to coverages &theta;=0.5 and &theta;=0.75&thinsp;monolayers are sketched in their stability domain (the black box indicates the surface unit cell). On the right panel the simulated STM images are shown for the &theta;&thinsp;=&thinsp;0.75 monolayer pattern for three different tip heights and a bias voltage V&thinsp;=&thinsp;&minus;1&thinsp;eV [1].</div> Zoom Image
Figure 2: The left panel shows the stability ranges for the most stable adsorption patterns/coverages of Se on the Mo(110) surface in equilibrium with a gas of Se2 molecules. The patterns corresponding to coverages θ=0.5 and θ=0.75 monolayers are sketched in their stability domain (the black box indicates the surface unit cell). On the right panel the simulated STM images are shown for the θ = 0.75 monolayer pattern for three different tip heights and a bias voltage V = −1 eV [1].
  • the interaction between the Mo back-contact and the MoSe2 layer (see Figure 3) forming between the Mo surfaces and the light absorber layer, explicitly including the weak van der Waals forces into the calculations to describe the morphology of the Mo-MoSe2 interface, and to calculate its electronic properties
<div style="text-align: justify;"><strong>Figure 3:</strong> Crystal structure of bulk hexagonal MoSe<sub>2</sub> (a), where a trigonal prism is highlighted with black color as a structural unit with one Mo atom in the trigonal prismatic hole of six Se atoms. The (10-10) and (11-20) surfaces of MoSe<sub>2</sub> are shown in subfigures (b) and (c), respectively, where the slabs representing the surfaces are repeated periodically along the x and y directions, and the surfaces are perpendicular to the z axis.</div> Zoom Image
Figure 3: Crystal structure of bulk hexagonal MoSe2 (a), where a trigonal prism is highlighted with black color as a structural unit with one Mo atom in the trigonal prismatic hole of six Se atoms. The (10-10) and (11-20) surfaces of MoSe2 are shown in subfigures (b) and (c), respectively, where the slabs representing the surfaces are repeated periodically along the x and y directions, and the surfaces are perpendicular to the z axis.
 
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