Surface Study of Cu2SnS3 Using First-Principles Density Functional Theory

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dc.contributor.author Dahule, Rohit
dc.contributor.author Raghav, Abhishek
dc.contributor.author Hanindriyo, Adie Tri
dc.contributor.author Hongo, Kenta
dc.contributor.author Maezono, Ryo
dc.contributor.author Panda, Emila
dc.coverage.spatial United States of America
dc.date.accessioned 2021-05-14T05:18:49Z
dc.date.available 2021-05-14T05:18:49Z
dc.date.issued 2021-04
dc.identifier.citation Dahule, Rohit; Raghav, Abhishek; Hanindriyo, Adie Tri; Hongo, Kenta; Maezono, Ryo and Panda, Emila, "Surface study of Cu2SnS3 using first?principles density functional theory", Advanced Theory and Simulations, DOI: 10.1002/adts.202000315, Apr. 2021. en_US
dc.identifier.issn 2513-0390
dc.identifier.uri https://doi.org/10.1002/adts.202000315
dc.identifier.uri https://repository.iitgn.ac.in/handle/123456789/6504
dc.description.abstract Here, the electronic structure of monoclinic Cu2SnS3 (CTS) along with the surface energy and surface electronic structure of (200) and ( 1⎯⎯ 31) terminated surfaces are computed using density functional theory (DFT). Moreover, this computation is carried out using the Heyd–Scuseria–Ernzerhof (HSE) hybrid functional after geometry optimization of ions performed using local density approximation (LDA). Surface distortion is seen for both these considered CTS surfaces after geometrical optimization of these surface supercells. In (200) surface supercell, Cu and Sn atoms are seen to move inwards, and outwards respectively, whereas, for ( 1⎯⎯ 31) surface supercell, S atoms show high lateral displacement. Moreover, the relaxation effect of subsurface ions results in the displacement of 0.1 Å, which further reduced beyond the second layer for (200) surface supercell, whereas, ( 1⎯⎯ 31) surface shows the random displacement of the subsurface ions. Moreover, the surface energy of (200) and ( 1⎯⎯ 31) surfaces are calculated to be 0.0292 and 0.3106 eV Å−2, respectively, indicating (200) being the more stable CTS surface. Furthermore, the valence and conduction band edges of these surfaces are found to overlap, suggesting metallic characteristics for these surfaces contrary to the semiconducting behavior found for the bulk CTS (with the calculated band gap of 0.78 eV).
dc.description.statementofresponsibility by Rohit Dahule, Abhishek Raghav, Adie Tri Hanindriyo, Kenta Hongo, Ryo Maezono and Emila Panda
dc.language.iso en_US en_US
dc.publisher Wiley en_US
dc.subject Cu2SnS3 en_US
dc.subject density functional theory en_US
dc.subject surface electronic structures en_US
dc.subject surface energy en_US
dc.subject surface relaxation en_US
dc.title Surface Study of Cu2SnS3 Using First-Principles Density Functional Theory en_US
dc.type Article en_US
dc.relation.journal Advanced Theory and Simulations


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