Evidence map›Paper›PMID 39431072›Full record

ArticleACS omega2024

Surface Reconstruction and Layer-Dependent Semiconductor-to-Metal Transition of Zinc-Blende CdSe.

Yuexin Dong, Kaiyun Chen, Songrui Wei, Le Zhang, Haoxi Dong, Cunle Bo, Wangtu Huo

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Article in ACS omega, 2024. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Not yet cited in PubMed.

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5 · Who and what money

Authors and funding

7 authors.

Yuexin DongSchool of Material Science and Engineering, Northeastern University, Shenyang 110819, China.
Kaiyun ChenNorthwest Institute for Nonferrous Metal Research, Xi'an 710016, China.ORCID https://orcid.org/0000-0003-1974-9428
Songrui WeiCollege of Physics and Optoelectronic Engineering, State Key Laboratory of Radio Frequency Heterogeneous Integration, Shenzhen University, Shenzhen 518060, China.
Le ZhangMOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xian 710049, China.ORCID https://orcid.org/0000-0003-4522-1555
Haoxi DongMOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xian 710049, China.
Cunle BoMOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xian 710049, China.
Wangtu HuoNorthwest Institute for Nonferrous Metal Research, Xi'an 710016, China.

Funding

No grant is acknowledged in the PubMed record.

6 · The paper itself

Abstract

In this work, CdSe was taken as the representation to systematically investigate the (111) and (110) surface reconstructions, the electronic properties transition related to the layer size, and the corresponding physical mechanism through the density functional theory (DFT) calculation. For the (111) surface slab structure, the bulk truncated relaxation (BTR) surface and the honeycomb (HC) surface were carefully examined. The HC surface configuration, ignored by previous studies, is an energetically preferred surface compared to both the as-truncated and BTR configurations. Based on the HC surface, the band structure of the (111) surface shows a semiconductor character below four layers (4L). Surprisingly, the (111) CdSe turns metallic in the 4L system. In a higher-layer (>4L) system, the two side surfaces and internal regions show metallic and semiconductivity features, respectively. Such an abundant electronic properties transition should be attributed to the electron transfer under the intrinsic polarization perpendicular to the asymmetrical (111) plane. Different from the (111) surface, drastic structural reconstructions were not observed in the (110) surface and the band gap gradually decreased with the increasing number of layers until it approached the value in the bulk. Our results not only revealed the additional possible surface structure but also clarified the underlying mechanism of semiconductor-to-metal (even the edge metallic) transition related to the number of layers. All these findings could be extended to other II-VI group MX compounds for further development of electronic devices.

Identifiers

PMID39431072
PMCPMC11483908

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