2017
DOI: 10.1016/j.jpcs.2017.04.006
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First principles calculation of interfacial stability, energy and electronic properties of SiC/ZrB 2 interface

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Cited by 45 publications
(18 citation statements)
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“…Figure 1 displays the interface structure of the Ge(111)/4H-SiC(0001) heterojunction based on the TEM characterizations [3]. The primitive cells of Ge(111) surface and 4H-SiC(0001) surface possess lattice constants of [01-1] Ge = 4.000Å, [11][12][13][14][15][16][17][18][19][20] SiC = 3.078Å. The lattice matching is 3 : 4 of Ge to SiC with a residual mismatch of 2.60% in the two parallel orientations using the smallest supercell mismatch.…”
Section: Resultsmentioning
confidence: 99%
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“…Figure 1 displays the interface structure of the Ge(111)/4H-SiC(0001) heterojunction based on the TEM characterizations [3]. The primitive cells of Ge(111) surface and 4H-SiC(0001) surface possess lattice constants of [01-1] Ge = 4.000Å, [11][12][13][14][15][16][17][18][19][20] SiC = 3.078Å. The lattice matching is 3 : 4 of Ge to SiC with a residual mismatch of 2.60% in the two parallel orientations using the smallest supercell mismatch.…”
Section: Resultsmentioning
confidence: 99%
“…All the calculations in this work were implemented by using the Cambridge Serial Total Energy Package (CASTEP) Code [12,13], which are based on the density functional theory (DFT) [14]. Generalized gradient approximation (GGA) of Perdew-Burke-Ernzerhof (PBE) scheme was employed to describe the exchange-correlation functional [15].…”
Section: Methodsmentioning
confidence: 99%
“…In the first principle calculation, the four models ( Figure 9) of the ZrB 2 (001)/Mo (110) interface are established according to the XRD results, and the interface properties of the model are effectively analyzed by the density functional theory (in order to ensure that the interface of the two parts fully represented the performance of the bulk material, through the surface energy convergence test, we selected, for both ZrB 2 and Mo, an atomic layer thickness of 9 layers, a cutoff energy of 450 eV, K point was 6 × 6 × 6, and the energy error was within 1-2 MeV/atom). In addition, the interface energy (γint) and ideal cohesion energy (W ad ) can be used to evaluate the bonding strength and stability of the interface [42]. So, we calculate the four models of ideal interface viscous work and the interface spacing (as shown in Table 1).…”
Section: Mechanism Of Friction Behaviormentioning
confidence: 99%
“…In the charge density differences (Figure 11b) of the ZrB 2 /Mo interface (Model 2), it shows that due to the interaction of interface layer atoms, Mo-Mo is obviously stretched out for a certain distance. Therefore, a part of the Mo-Mo region is close to the B direction, and then part of the charges of the Mo atoms at the interface are transferred to the interface B atoms to form the ionic bonds, that is, the strong interaction between B and Mo [42,44]. In addition, from the perspective of charge accumulation, the charges are mainly concentrated near the B layer.…”
Section: Mechanism Of Friction Behaviormentioning
confidence: 99%
“…Therefore, NbC (111) and TiC (111) with thicknesses larger than thirteen atomic layers were chosen to construct the interfaces in the following calculations. The surface energies of NbC and TiC were calculated using the method of Shi et al [16,31], and the results are shown in Figure 1a,b respectively. It is found that the surface energies of Nbterminated and C-terminated NbC (111) are 1.75-2.88 and 5.70-6.83 J/m 2 , respectively.…”
Section: Surface Properties Of Nbc and Ticmentioning
confidence: 99%