Abstract:Structural, electronic and magnetic properties were calculated for the optimized α-U/W(110) thin films (TFs) within the density functional theory. Our optimization for 1U/7W(110) shows that the U-W vertical interlayer spacing (ILS) is expanded by 14.0% compared to our calculated bulk W-W ILS. Spin and orbital magnetic moments (MMs) per U atom were found to be enhanced from zero for the bulk of α-U to 1.4 µB and -0.4 µB at the interface of the 1U/7W(110), respectively. Inversely, our result for 3U/7W(110) TFs s… Show more
“…The equilibrium primitive unit cell volumes were 0.02015 and 0.01606 nm 3 , respectively. These results were in agreement with the pseudopotential results of the others [19][20][21][22][23], as well as experimental results in Refs. [24,25].…”
Section: Computational and Experimental Methodssupporting
confidence: 93%
“…Relaxation continues until the optimization is completed and the lowest energy interface is the reasonable distance, 0.24 nm, as listed in Table 2. According to the computational result and Zarshenas' investigation [23], a crystal orientation of W(110)/ a-U(001) was selected. Although other kinds of interface orientations between bcc-W and orthorhombic a-U can be presented, it is believed that the primary bonding can be characterized by a model as investigated in this study.…”
Section: U/w Interface Structure and Preference Sitementioning
The stability, bonding, work of adhesion and electronic structure of the U/W interface with and without Ti were investigated by first principles to explore the mechanical properties of W particles enhanced U-Ti alloy matrix composite as a construction material. The calculated results indicate that the preferable orientation of the U/W interfacial structure is (001) U /(110) W crystallographic plane, Ti atoms originating from U slab are prone to diffuse into W slab through the interface, and additional Ti in U matrix is the stronger adhesion to W, with an ideal work of adhesion of 6.93 JÁm -2 for U-Ti/W interface, relative to the value of 6.72 JÁm -2 for clean U/W interface. The stronger adhesion performance is due to the increase in valence electron hybridization for U-Ti/W compared with U/W interface, as evidenced by the characteristic of the local density of states for the interfacial atoms.
“…The equilibrium primitive unit cell volumes were 0.02015 and 0.01606 nm 3 , respectively. These results were in agreement with the pseudopotential results of the others [19][20][21][22][23], as well as experimental results in Refs. [24,25].…”
Section: Computational and Experimental Methodssupporting
confidence: 93%
“…Relaxation continues until the optimization is completed and the lowest energy interface is the reasonable distance, 0.24 nm, as listed in Table 2. According to the computational result and Zarshenas' investigation [23], a crystal orientation of W(110)/ a-U(001) was selected. Although other kinds of interface orientations between bcc-W and orthorhombic a-U can be presented, it is believed that the primary bonding can be characterized by a model as investigated in this study.…”
Section: U/w Interface Structure and Preference Sitementioning
The stability, bonding, work of adhesion and electronic structure of the U/W interface with and without Ti were investigated by first principles to explore the mechanical properties of W particles enhanced U-Ti alloy matrix composite as a construction material. The calculated results indicate that the preferable orientation of the U/W interfacial structure is (001) U /(110) W crystallographic plane, Ti atoms originating from U slab are prone to diffuse into W slab through the interface, and additional Ti in U matrix is the stronger adhesion to W, with an ideal work of adhesion of 6.93 JÁm -2 for U-Ti/W interface, relative to the value of 6.72 JÁm -2 for clean U/W interface. The stronger adhesion performance is due to the increase in valence electron hybridization for U-Ti/W compared with U/W interface, as evidenced by the characteristic of the local density of states for the interfacial atoms.
“…Therefore, the LaIn 3 and LaSn 3 compounds show more ductility than the remaining RIn 3 and RSn 3 compounds, which is due to the large separation between the Fermi level and the f states according to a previous study. 50 Strongly correlated systems such as lanthanides (and actinides) 39,51 which involve 4f (or 5f) orbitals have interesting physical and chemical properties, because these electrons can be localized or itinerant depending on the crystalline environment. Therefore, to understand the effects of the 4f orbitals in these compounds, the calculations are also carried out with the Hubbard potential U (GGA + U and LDA + U).…”
Section: B Electronic Structure and Density Of Statesmentioning
The cubic rare-earth intermetallics RIn3 and RSn3 (R = La, Ce, Pr, Nd) have been investigated using the full potential linearized augmented plane waves plus local orbital method in the density functional theory framework.
“…According to the Hill criteria, 20 uranium based compounds with the U-U interatomic distances smaller than 3.4-3.6 Å are typically nonmagnetic with itinerant 5f states. 21 Metallic uranium is paramagnetic but shows magnetic ordering when it combines with group 5 (N, P, As, Sb, Bi) or group 6 (S, Se, Te) elements. All UX 2 (X ¼ Bi, Sb, As, P) actinide compounds are antiferromagnetic with relatively high Néel temperature.…”
In this paper, we explore the electric field gradients (EFGs) at 238U sites for antiferromagnetic UX2 (X = P, As, Sb, Bi) dipnicties using LDA, LDA + U, GGA, GGA + U, and EECE schemes in the presence of spin–orbit coupling.
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