Electronic structure and the ground-state properties of cobalt antimonide skutterudites: Revisited with different theoretical methods

2012 ◽  
Vol 210 (1) ◽  
pp. 131-139 ◽  
Author(s):  
Lukas Hammerschmidt ◽  
Sabine Schlecht ◽  
Beate Paulus
1988 ◽  
Vol 153-155 ◽  
pp. 1215-1216 ◽  
Author(s):  
G. Malcolm Stocks ◽  
W.M. Temmerman ◽  
Z. Szotek ◽  
G.Y. Guo ◽  
P.J. Durham

2015 ◽  
Vol 51 (67) ◽  
pp. 13178-13180 ◽  
Author(s):  
Xueliang Shi ◽  
Sangsu Lee ◽  
Minjung Son ◽  
Bin Zheng ◽  
Jingjing Chang ◽  
...  

A pro-aromatic molecule BPT-TIPS displayed different ground-state electronic structure and physical properties from its anti-aromatic counterpart S2-TIPS.


2013 ◽  
Vol 665 ◽  
pp. 43-48
Author(s):  
Rajagopalan Umamaheswari ◽  
M. Yogeswari ◽  
G. Kalpana

The first-principles calculation within density functional theory is used to study in detail the electronic structure and ground state properties of alkali-metal oxoargenates A4[Ag4O4] (A= Na, K and Rb). The total energies calculated within the atomic sphere approximation (ASA) were used to determine the ground state properties such as equilibrium lattice parameter, c/a ratio, bulk modulus and cohesive energy. The theoretically calculated equilibrium lattice constants values are in well agreement with the available experimental values. The electronic band structures, total and partial density of states are calculated. The result of electronic band structure shows that the KAgO and RbAgO are direct band gap semiconductors with their gap lying between the Γ-Γ points, whereas NaAgO is found to be an indirect band gap semiconductor with its gap lying between Z-Γ points.


2003 ◽  
Vol 17 (25) ◽  
pp. 4447-4456 ◽  
Author(s):  
DURGA PAUDYAL ◽  
ABHIJIT MOOKERJEE

We have studied the electronic properties like density of states and band structures and also the ground state properties like formation energy, cohesive energy, bulk modulus and structural energy of NiPt system using the linearized muffin-tin orbital method introduced by Andersen.1,2 In an earlier communication we had argued that both charge neutrality and scalar relativistic corrections are very important for the high concentration of Pt alloys. The calculations here, were, therefore, carried out with charge neutrality as well as with and without scalar relativistic correction for comparison.


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