Fermi-level Unpinning at Sn/Ge Interfaces; First-principles Calculation

The electronic structure and magnetic properties of C atoms in Co, Ni-substituted graphene single-layers were studied by first-principles calculation method based on density functional theory. The study found that the pure graphene single-layer is an insulator, does not have magnetism, and we found that the doping of Co and Ni atoms alone does not make the system magnetic. Both Co and Ni atoms are capable of generating impurity levels in the graphene single-layer system. The impurity level of Co atom doping is 0.75 eV below the Fermi level, and the impurity level of Ni atom doping is 0.4 eV above the Fermi level. Studies on the coupling doping of Co and Ni atoms show that two different distance Co atoms or Ni atoms in the graphene single-layer are not always ferromagnetically coupled, and a stable magnetic ground state cannot be obtained. It can produce different magnetic ground states by controlling different doping distances, thus we provide one new way to control the spin properties.

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First-principles study on the electronic and magnetic properties of the Zn0.75Mo0.25M(M = S,Se,Te)

Modern Physics Letters B ◽

10.1142/s0217984916502493 ◽

2016 ◽

Vol 30 (19) ◽

pp. 1650249 ◽

Cited By ~ 4

Author(s):

Zhu-Hua Yin ◽

Jian-Min Zhang ◽

Ke-Wei Xu

Keyword(s):

Magnetic Properties ◽

Fermi Level ◽

First Principles ◽

Atomic Radius ◽

Band Gaps ◽

First Principles Calculation ◽

Spintronic Devices ◽

Lattice Constants ◽

Electronic And Magnetic Properties ◽

Tetrahedral Crystal

The geometrical, electronic and magnetic properties of the Zn[Formula: see text]Mo[Formula: see text]M (M[Formula: see text]=[Formula: see text]S, Se and Te) have been studied by spin-polarized first-principles calculation. The optimized lattice constants of 5.535, 5.836 and 6.274 Å for M[Formula: see text]=[Formula: see text]S, Se and Te are related to the atomic radius of 1.09, 1.22 and 1.42 Å for S, Se and Te atoms, respectively. The Zn[Formula: see text]Mo[Formula: see text]M are magnetic half-metallic (HM) with the spin-down conventional band gaps of 2.899, 2.126 and 1.840 eV, while the HM band gaps of 0.393, 0.016 and 0.294 eV for M[Formula: see text]=[Formula: see text]S, Se and Te, respectively. At the Fermi level, the less than half-filled Mo-[Formula: see text] orbital hybridizated with the less M-[Formula: see text] orbital contributes only spin-up channel leading Zn[Formula: see text]Mo[Formula: see text]M an HM ferromagnetism. The tetrahedral crystal field formed by adjacent three Zn atoms and one M atom splits the spin-up channel (majority spin) of Mo-[Formula: see text] orbital into three-fold degenerate [Formula: see text] states at the Fermi level and double degenerate [Formula: see text] [Formula: see text] states below the Fermi level. The exchange splitting energies of the Zn[Formula: see text]Mo[Formula: see text]M are −2.611, −2.231 and −1.717 eV for M[Formula: see text]=[Formula: see text]S, Se and Te, respectively. The results provide an useful theoretical guidance for Zn[Formula: see text]Mo[Formula: see text]M applications in spintronic devices.

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An Investigation on Substitution of Ag Atoms for Al or Ti Atoms in the Ti2AlC MAX Phase Ceramic Based on First-Principles Calculations

Materials ◽

10.3390/ma14227068 ◽

2021 ◽

Vol 14 (22) ◽

pp. 7068

Author(s):

Guochao Wang ◽

Jiahe Zhou ◽

Weijian Chen ◽

Jianguo Yang ◽

Jie Zhang ◽

...

Keyword(s):

Electrical Conductivity ◽

Fermi Level ◽

First Principles ◽

First Principles Calculation ◽

Max Phase ◽

Lattice Stability ◽

Substitution Ratio ◽

New Perspective ◽

The Stability ◽

Bonding Characteristic

The present work introduced first-principles calculation to explore the substitution behavior of Ag atoms for Al or Ti atoms in the Ti2AlC MAX phase ceramic. The effect of Ag substitution on supercell parameter, bonding characteristic, and stability of the Ti2AlC was investigated. The results show that for the substitution of Ag for Al, the Al-Ti bond was replaced by a weaker Ti-Ag bond, decreasing the stability of the Ti2AlC. However, the electrical conductivity of the Ti2AlC was enhanced after the substitution because of the contribution of Ag 4d orbital electrons toward the density of states (DOS) at the Fermi level coupled with the filling of Ti d orbital electrons. For the substitution of Ag for Ti, new bonds, such as Ag-Al bond, Ag-C bond, Al-Al bond, Ti-Ti anti-bond, and C-C anti-bond were generated in the Ti2AlC. The Ti-Ti anti-bond was strengthened as well as the number of C-C anti-bond was increased with increasing the substitution ratio of Ag for Ti. Similar to the substitution of Ag for Al, the stability of the Ti2AlC also decreased because the original Al-Ti bond became weaker as well as the Ti-Ti and C-C anti-bonds were generated during the substitution of Ag for Ti. Comparing with the loss of Ti d orbital electrons, Ag 4d orbits contributed more electrons to the DOS at the Fermi level, improving the electrical conductivity of the Ti2AlC after substitution. Based on the calculation, the substitution limit of Ag for Al or Ti was determined. At last, the substitution behavior of Ag for Al or Ti was compared to discriminate that Ag atoms would tend to preferentially substitute for Ti atoms in Ti2AlC. The current work provides a new perspective to understand intrinsic structural characteristic and lattice stability of the Ti2AlC MAX phase ceramic.

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