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Fermi radius

The Fermi energy, and hence the Fermi radius must be a function of r,... [Pg.349]

We have set, in the above derivation, r — r where the Fermi radius is... [Pg.53]

The Fe-Mn alloys (2-8-6-7 at. % Mn) have many similarities to the Fe-Al system [36], with the exception that the conduction-electron spin-density oscillations show a phase variation with concentration corresponding to a change in the Fermi radius and band structure (see Figs. 11.5 and 11.6) [32]. In this case the Mn atoms are contributing to the.magnetic structure. [Pg.314]

Within a jellium atom, the electron frequency is of order 1017/sec. compared with the plasmon frequency for jellium (1.1 x 1016/sec.) so an isolated jellium atom behaves as a dielectric. However, the valence electron screens any electric field caused by polarization. The screening length (Thomas-Fermi) is 0.47Ang., or 0.36 of the radius of the jellium atom. Thus the field of the positive ion is reduced by about 30% at R. [Pg.44]

The electrons that occupy the levels of a Fermi gas have energies < and may be considered as confined to a (Fermi) sphere of radius kF in k-space. For large volumes the free-electron quantum numbers may be treated as continuous variables and the number of states in a range dk = dkxdkydkz, is... [Pg.305]

Therefore the main assumptions of this approach, provided that such matching radius rg exists, can be summarized as i) for r > rg the system is adequately described as a local relativistic Fermi gas, ii) for r< rg the main contribution is due to the U singleparticle state, and iii) the potential near the nucleus is approximated to - )/r. In addition to this, exchange effects were not considered. [Pg.198]

The Fermi energy ej is found by imposing that at the cutoff radius the potential... [Pg.206]

Substituting for r the radius of the Fermi sphere = 3/4jt p) we can rewrite the kinetic energy as ... [Pg.184]

The function fct d) has no physical basis. According to Heiden (6), it should fulfill only two conditions it should be smooth and continuous and have finite values for d < dcut oS. The value of dclH 0[f should be larger than the van der Waals radius of any atom in the molecule under consideration. In the program LipoDyn, the Ghose and Crippen parameters (18) as well as the Broto and Moreau parameter set (16) are implemented, with the the exponential function used by Fauchere (cxp(-d)) (3), the hyperbolic function defined by Audry 1/(1 + d) (2) and the parameterized Fermi distance function used by Testa and coworkers (1). [Pg.220]

In the s-wave-tip model (Tersoff and Hamann, 1983, 1985), the tip was also modeled as a protruded piece of Sommerfeld metal, with a radius of curvature R, see Fig. 1.25. The solutions of the Schrodinger equation for a spherical potential well of radius R were taken as tip wavefunctions. Among the numerous solutions of this macroscopic quantum-mechanical problem, Tersoff and Hamann assumed that only the s-wave solution was important. Under such assumptions, the tunneling current has an extremely simple form. At low bias, the tunneling current is proportional to the Fermi-level LDOS at the center of curvature of the tip Pq. [Pg.28]

Another example in Fig. 6.3 is the image of the Au(lll) surface with a step, as observed by W611 et al. (1989). Direct measurement gives an apparent radius of 1.5-2.0 A. At the Fermi level, the electronic states of a gold surface are dominated by i atomic states. The closest tip-sample distance that is possible experimentally is 3 A. Therefore, the tip state is likely to be a d state. [Pg.157]

Suppose we take an electron out of one of the hydrogen atoms, leaving behind a H ion. The electron will be re-attracted to the ion by a potential - e /R. It will be bound in the ground state for this potential, which has a radius Uh = h /me. If, however, there are enough ionized electrons in the lattice, they will screen the electron from the positive ion core, according to a potential - (e /R) exp(- kR), where X is a screening parameter in the Thomas-Fermi modeP X... [Pg.38]

Thus, although it is safe to assume that the 5f states are localized states, excited f states are never far above the Fermi energy. They will, therefore, influence the electronic properties and high temperature phases of Cf and Es (which, with a metal radius R = 2.0 A seem to have attained divalency). [Pg.47]


See other pages where Fermi radius is mentioned: [Pg.317]    [Pg.306]    [Pg.378]    [Pg.397]    [Pg.317]    [Pg.306]    [Pg.378]    [Pg.397]    [Pg.115]    [Pg.220]    [Pg.816]    [Pg.40]    [Pg.49]    [Pg.322]    [Pg.33]    [Pg.55]    [Pg.67]    [Pg.67]    [Pg.266]    [Pg.191]    [Pg.237]    [Pg.269]    [Pg.271]    [Pg.254]    [Pg.17]    [Pg.308]    [Pg.49]    [Pg.183]    [Pg.31]    [Pg.165]    [Pg.232]    [Pg.18]    [Pg.198]    [Pg.198]    [Pg.19]    [Pg.31]    [Pg.157]    [Pg.109]   
See also in sourсe #XX -- [ Pg.349 ]




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Thomas Fermi radius

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