Electronic and elastic properties of two new B-C-N superhard materials from first principles

2021 ◽  
Vol 340 ◽  
pp. 114520
Author(s):  
Chenchen Jing ◽  
Liwei Shi ◽  
Yang Zhang ◽  
Fan Yuan ◽  
Xinyue Qian
Keyword(s):  
Elastic Properties ◽  
First Principles ◽  
Superhard Materials

First-principles study of (Ti5−xMgx)Si3 phases with the hexagonal D88 structure: Elastic properties and electronic structure

2012 ◽  
Vol 54 ◽  
pp. 287-292 ◽  
Author(s):  
Xiao-Jun Chen ◽  
Meng-Xue Zeng ◽  
Ren-Nian Wang ◽  
Zhou-Sheng Mo ◽  
Bi-Yu Tang ◽  
...  
Keyword(s):  
Electronic Structure ◽  
Elastic Properties ◽  
First Principles ◽  
First Principles Study

First principles study on electronic structure and elastic properties of LaCd and LaHg

2014 ◽  
Author(s):  
Hansa Devi ◽  
Gitanjali Pagare ◽  
S. S. Chouhan ◽  
Sankar P. Sanyal
Keyword(s):  
Electronic Structure ◽  
Elastic Properties ◽  
First Principles ◽  
First Principles Study

First-principles study of electronic structure, chemical bonding and elastic properties for new superconductor CaFeAs2

2017 ◽  
Vol 31 (02) ◽  
pp. 1650263
Author(s):  
J. G. Yan ◽  
Z. J. Chen ◽  
G. B. Xu ◽  
Z. Kuang ◽  
T. H. Chen ◽  
...  
Keyword(s):  
Electronic Structure ◽  
Elastic Properties ◽  
Density Of States ◽  
First Principles ◽  
Elastic Anisotropy ◽  
First Principles Calculation ◽  
Hard Material ◽  
Dirac Cone ◽  
First Time ◽  
New Superconductor

Using first-principles calculation we investigated the structural, electronic and elastic properties of paramagnetic CaFeAs2. Our results indicated that the density of states (DOS) was dominated predominantly by Fe-3[Formula: see text] states at Fermi levels, and stronger hybridization exists between As1 and As1 atoms. Three hole pockets are formed at [Formula: see text] and Z points, and two electronic pockets are formed at A and E points. The Dirac cone-like bands appear near B and D points. For the first time we calculated the elastic properties and found that CaFeAs2 is a mechanically stable and moderately hard material, it has elastic anisotropy and brittleness, which agrees well with the bonding picture and the calculation of Debye temperature ([Formula: see text]).

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