The total electronic band structure energy for 29 elements

The total electronic band structure energy is calculated for 29 elements by the method of the screened model potential of Heine & Abarenkov (1964). The division of the total energy of a metal into free electron, band structure, and electrostatic parts follows the method initiated by Harrison (1963) for the calculation of atomic properties. By drawing an analogy with the procedure introduced by Cochran (1963) for the experimental determination of the electronic contribution to phonon spectra of metals, we arrive at a more convenient expression for the total band structure energy in a form applicable to the determination of atomic properties, phonon spectra, general interatomic forces, and possibly liquid metal properties. Numerical results are compared with those derived from experiment and from the o. p. w. pseudopotential method.

2007 ◽  
Vol 91 (14) ◽  
pp. 142121 ◽  
Author(s):  
Z. H. Wu ◽  
F. A. Ponce ◽  
Joachim Hertkorn ◽  
Ferdinand Scholz

RSC Advances ◽  
2019 ◽  
Vol 9 (2) ◽  
pp. 1134-1146 ◽  
Author(s):  
Yin Zhang ◽  
Jose A. Alarco ◽  
Adam S. Best ◽  
Graeme A. Snook ◽  
Peter C. Talbot ◽  
...  

The surface Li depletion affects the determination of optical gap for LiFePO4, which was previously used for validation of DFT calculations.


1993 ◽  
Vol 46 (5) ◽  
pp. 717 ◽  
Author(s):  
Robert Leckey ◽  
John Riley ◽  
Yong Cai ◽  
Jurgen Faul ◽  
Lothar Ley

Both the calculation and the experimental determination of the band structure of simple materials using the techniques of photoemission have now reached levels of considerable sophistication and maturity. Indeed, it is often claimed that the determination of the detailed electronic band structure of semiconductors, for example, is almost routine using angle-resolved photoelectron spectroscopy in conjunction with synchrotron radiation. In this paper we will discuss the extent to which this claim is justified, illustrating the discussion with recent results from a number of III/V semiconductors. We will demonstrate the model-dependent nature of current interpretations of the experimental data, and will show that the technique is presently limited due to the scarcity of information concerning excited band states well above the vacuum level.


1980 ◽  
Vol 35 (1) ◽  
pp. 69-71 ◽  
Author(s):  
H. Asonen ◽  
M. Lindroos ◽  
M. Pessa ◽  
N. Dahlbäck

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