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Transition metal 5 band

The behaviour of the transition-metal bands as the atoms are brought together to form the solid may be evaluated within the Wigner-Seitz sphere approximation by imposing bonding, = 0, or antibonding, R, = 0,... [Pg.180]

We see clearly why so many parameters have been required in fitting the transition-metal bands. Our formulation was based initially upon the parameters Kw., K,.,, Kv.., and - c,. (The parameter K... [Pg.484]

Much insight in the transition metal band structure is provided by the LMTO method (Andersen 1975, Andersen and Jepsen 1977, Andersen et al. 1985, Skriver 1983a), which gives a very useful approximate description of narrow transition-metal bands when they hybridize little with s and p bands. The unhybridized energy band eigenvalues given by eq. (22) become particularly simple when y, is small. Then... [Pg.169]

R. L. Jacobs, The theory of transition metal band structures, J. Phys. C1,492-506 (1968). [Pg.109]

Simple metals like alkalis, or ones with only s and p valence electrons, can often be described by a free electron gas model, whereas transition metals and rare earth metals which have d and f valence electrons camiot. Transition metal and rare earth metals do not have energy band structures which resemble free electron models. The fonned bonds from d and f states often have some strong covalent character. This character strongly modulates the free-electron-like bands. [Pg.129]

Massidda S, Continenza A, Posternak M and Baldereschi A 1997 Quasiparticle energy bands of transition-metal oxides within a model GW scheme Phys. Rev. B 55 13 494-502... [Pg.2230]

Terakura K, Williams A R, Qguchi T and Kubler J 1984 Transition-metal monoxides Band or Mott insulators Phys. Rev. Lett. 52 1830... [Pg.2230]

Terakura K, Qguchi T, Williams A R and Kubler J 1984 Band theory of insulating transition-metal monoxides Band-structure calculations Phys. Rev. B 30 4734... [Pg.2230]

Fig. 12. The relationship between the mean oceanic residence time, T, yr, and the seawater—cmstal rock partition ratio,, of the elements adapted from Ref. 29. , Pretransition metals I, transition metals , B-metals , nonmetals. Open symbols indicate T-values estimated from sedimentation rates. The sohd line indicates the linear regression fit, and the dashed curves show the Working-Hotelling confidence band at the 0.1% significance level. The horizontal broken line indicates the time required for one stirring revolution of the ocean, T. ... Fig. 12. The relationship between the mean oceanic residence time, T, yr, and the seawater—cmstal rock partition ratio,, of the elements adapted from Ref. 29. , Pretransition metals I, transition metals , B-metals , nonmetals. Open symbols indicate T-values estimated from sedimentation rates. The sohd line indicates the linear regression fit, and the dashed curves show the Working-Hotelling confidence band at the 0.1% significance level. The horizontal broken line indicates the time required for one stirring revolution of the ocean, T. ...
The colors obtained depend primarily on the oxidation state and coordination number of the coloring ion (3). Table 1 Hsts the solution colors of several ions in glass. AH of these ions are transition metals some rare-earth ions show similar effects. The electronic transitions within the partially filled d andy shells of these ions are of such frequency that they fall in that narrow band of frequencies from 400 to 700 nm, which constitutes the visible spectmm (4). Hence, they are suitable for producing color (qv). [Pg.425]

The general understanding of the electronic structure and the bonding properties of transition-metal silicides is in terms of low-lying Si(3.s) and metal-d silicon-p hybridization. There are two dominant contributions to the bonding in transition-metal compounds, the decrease of the d band width and the covalent hybridization of atomic states. The former is caused by the increase in the distance between the transition-metal atoms due to the insertion of the silicon atoms, which decreases the d band broadening contribution to the stability of the lattice. [Pg.191]

We will limit ourselves to the surface segregation energy of an impurity of atomic number Z + 1 in a BCC matrix of atomic number Z and study the variation of this energy as a function of the number Nj of d electrons per atom in the d band of e transition metal Z. [Pg.376]

The surface have been assumed, unrelaxed and unreconstructed. The d band filling has been varied in the range (3 - 4.6)e per atom which includes the BCC transition metals and, in particular, the case of Ta and W. The results are displayed in Fig. 2. As often assumed, we have taken Nd(Z + 1) - Nd(Z) = 1.1. However, as shown in Fig. 2, changing this difference to 1 modifies only slightly the numerical results. [Pg.377]


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