
Half-metallic magnetism and electronic structures of CrPSe<sub>3</sub> monolayers with multiple Dirac cones<span style="background-color: rgb(255, 255, 255);"><span style="color:#ff0000;">(withdraw)</span></span>
Author(s) -
Yang Jun-Tao,
Xiong Yong-Chen,
Huang Hai-Ming,
Luo Shi-Jun
Publication year - 2020
Publication title -
wuli xuebao
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.199
H-Index - 47
ISSN - 1000-3290
DOI - 10.7498/aps.69.20200960
Subject(s) - superexchange , physics , condensed matter physics , ground state , ferromagnetism , magnetism , monolayer , materials science , atomic physics , nanotechnology
According to the first-principles calculation within PBE+ U method and tight-binding model, the magnetic properties and electronic structures of two-dimensional (2D) CrPSe 3 monolayer were investigated. Constructed by a Cr-honeycomb hexagonal lattice, 2D CrPSe 3 was predicted to be in a half-metallic ferromagnetic state with dynamic stability, confirmed by the phonon spectrum with no imaginary dispersion. The Curie temperature was estimated as 224 K by Monte Carlo simulation within the Metropolis algorithm under the periodic boundary condition. The thermal stability of CrPSe 3 monolayer was estimated at 300 K by a first-principles molecular dynamics simulation. It is found that the magnetic ground state of CrPSe 3 monolayer is determined by a competition between the antiferomagnetic d-d direct exchange interactions and the Se-p orbitals mediated ferromagnetic p-d superexchange interactions. Most interestingly, in the half-metallic state the band structure exhibits multiple Dirac cones in the first Brillouin zone: two cones at K point showing a very high Fermi velocity \begin{document}${v_{\rm F}{(K)}} = 15.8 \times 10^5 \;{\rm m \!\cdot\! s^{-1}}$\end{document}about twice larger than the \begin{document}$ v_{\rm F} $\end{document}of graphene in the vicinity of Fermi level, and six cones at \begin{document}$ K'/2 $\end{document}points with \begin{document}${ v_{\rm F} {(K'/2)}} = 10.1 \times 10^5\;{\rm m \!\cdot\! s^{-1}}$\end{document}close to the graphene's value. These spin-polarized Dirac cones are mostly composed of Cr \begin{document}${\rm d}_{xz}$\end{document}and \begin{document}${\rm d}_{yz}$\end{document}orbitals. The novel electronic structure of CrPSe 3 monolayer is also confirmed by the HSE06 functional. A tight-binding model was built based on the Cr-honeycomb structure with two Cr-d orbitals as the basic with the first, second and third nearest-neighboring interactions, further demonstrating that the multiple Dirac cones are protected by the Cr-honeycomb lattice symmetry. Our findings indicate that 2D CrPSe 3 monolayer is a candidate with potential applications in the low-dimensional, high speed and temperature spintronics.