Novel BCN2 and CN compounds in C2/m phase: First-principle calculations

被引:8
|
作者
Liu, Yonghong [1 ]
Li, Xiaozhen [2 ]
Xing, Mengjiang [3 ]
Jin, Jianhui [1 ]
机构
[1] Kunming Univ Sci & Technol, Fac Informat Engn & Automat, Kunming 650500, Yunnan, Peoples R China
[2] Kunming Univ, Dept Informat & Technol, Kunming 650214, Yunnan, Peoples R China
[3] Univ Elect Sci & Technol China, Sch Microelect & Solid State Elect, Chengdu 610054, Peoples R China
基金
中国国家自然科学基金;
关键词
CN; BCN2; Metallic; Superhard material; Mechanical anisotropy; ELECTRONIC-PROPERTIES; THERMODYNAMIC PROPERTIES; CARBON ALLOTROPE; SUPERHARD PHASE; BORON-NITRIDE; CRYSTALS; HARDNESS;
D O I
10.1016/j.jpcs.2021.110231
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
A novel superhard CN (the stoichiometric ratio of carbon to nitrogen is 1:1) and BCN2 compound in C2/m phase are proposed and predicted according to density functional theory in this work. The physical properties, such as crystal structure, electronic properties, elastic properties, mechanical anisotropy properties and the stable of CN and BCN2 are investigated. The shear modulus G, Young's modulus E, and bulk modulus B of BCN2 and CN are 253 and 310 GPa; 448 and 719 GPa; and 186 and 323 GPa with GGA functional, respectively. Utilizing the Lyakhov-Oganov's model, CN and BCN2 are superhard materials, the hardness of CN and BCN2 is 60.99 GPa and 53.38 GPa, respectively. Compared with diamond and c-BN, although the hardness of CN and BCN2 is not as great as that of diamond, while they are both greater than that of c-BN. Using the Chen's model, CN also is a super-hard material with hardness is 58.63 GPa, while the hardness of BCN2 is only 26.67 GPa. C2/m CN is an indirect and wide band gap semiconductor material, while BCN2 is a metallic material. In addition, mechanical anisotropy of shear modulus G, Young's modulus E, and bulk modulus B of CN and BCN2 are also studied in detail.
引用
收藏
页数:10
相关论文
共 50 条
  • [1] Origin of direct band gap of Li2CN2 studied by first-principle calculations
    Kushida, Kazumasa
    Kuriyama, Kazuo
    [J]. PHYSICA B-CONDENSED MATTER, 2020, 598
  • [3] First-Principle Calculations of Hardness and Melting Point of Mo2C
    Wang, X. R.
    Yan, M. F.
    Chen, H. T.
    [J]. JOURNAL OF MATERIALS SCIENCE & TECHNOLOGY, 2009, 25 (03) : 419 - 422
  • [4] First-principle calculations of ternary compounds: Immm-BxTi3-xN2
    Wang, Xin-Kuan
    Yang, Ruike
    Ma, Shaowei
    Chai, Bao
    Xue, Minhua
    [J]. INTERNATIONAL JOURNAL OF MODERN PHYSICS B, 2019, 33 (25):
  • [5] First-principle calculation on the electronic structure of the molecule-based ferromagnet Co[P(CN)2]2 and M[N(CN)2]2 (M = Co, Ni)
    Zhu, L.
    Yao, K. L.
    Liu, Z. L.
    [J]. CHEMICAL PHYSICS LETTERS, 2006, 424 (1-3) : 209 - 213
  • [6] First-principle calculations of electronic and positronic properties of AlGaAS2
    Laref, S.
    Mecabih, S.
    Abbar, B.
    Bouhafs, B.
    Laref, A.
    [J]. PHYSICA B-CONDENSED MATTER, 2007, 396 (1-2) : 169 - 176
  • [7] First-principle calculations of the elastic properties of AIIBIVCV2 semiconductors
    Kumar, V.
    Singh, Bhanu P.
    Pandey, Bramha P.
    [J]. COMPUTATIONAL MATERIALS SCIENCE, 2014, 87 : 227 - 231
  • [8] Structural and Electronic Properties of LaPd2As2 Superconductor: First-Principle Calculations
    Singh, Birender
    Kumar, Pradeep
    [J]. 61ST DAE-SOLID STATE PHYSICS SYMPOSIUM, 2017, 1832
  • [9] First-principle calculations on Li2CuSb: A novel material for lithium-ion batteries
    Shukla, Ashutosh
    Pandey, Shail
    Pandey, Himanshu
    [J]. ENERGY STORAGE, 2023, 5 (02)
  • [10] First-principle calculations of magnetic properties of Ho6(Fe, Mn)Bi2 compounds
    Garcia-Adeva, Angel J.
    Apinaniz, Estibaliz
    Herrero, Aritz
    Aseguinolaza, Ivan R.
    Oleaga, Alberto
    [J]. RARE METALS, 2024,