scholarly journals Computing total energies in complex materials using charge self-consistent DFT + DMFT

2014 ◽  
Vol 90 (23) ◽  
Author(s):  
Hyowon Park ◽  
Andrew J. Millis ◽  
Chris A. Marianetti
2002 ◽  
Vol 20 (1) ◽  
pp. 139-144 ◽  
Author(s):  
R. RODRÍGUEZ ◽  
J.G. RUBIANO ◽  
J.M. GIL ◽  
P. MARTEL ◽  
E. MÍNGUEZ

In this work, a new analytical potential for studying ions in excited configurations is presented, which is built up from a parametric potential for ions in a ground state. It is used to calculate atomic magnitudes of special importance in plasmas such as total energies, energy levels, and transition energies, for ions in excited configurations. The results are successfully compared with those obtained with both self-consistent or analytical models.


1998 ◽  
Vol 58 (19) ◽  
pp. 12684-12690 ◽  
Author(s):  
Arno Schindlmayr ◽  
Thomas J. Pollehn ◽  
R. W. Godby

2018 ◽  
Vol 60 (9) ◽  
pp. 1641
Author(s):  
Л.Н. Граматеева ◽  
А.В. Лукоянов

AbstractThe electronic structure and the exchange interactions in EuNi_4Co and YbNi_4Co compounds have been calculated in terms of a theoretical approach with the inclusion of electronic correlations (LSDA + U method); the variants of substitution of cobalt ion for nickel in the 3 d lattice in both types of crystallographic positions 2 c and 3 g are considered. The total energies obtained in self-consistent calculations show that individual cobalt impurities are more preferably arranged in position of the 3 g type. A Co ion in RNi_4Co (R = Eu, Yb) is characterized by a significant magnetic moment, which leads to significant increase in the exchange interaction of Co and Ni ions in the 3 d metal sublattice.


1998 ◽  
Vol 58 (11) ◽  
pp. 7260-7268 ◽  
Author(s):  
M. Elstner ◽  
D. Porezag ◽  
G. Jungnickel ◽  
J. Elsner ◽  
M. Haugk ◽  
...  

1991 ◽  
Vol 253 ◽  
Author(s):  
Erik C. Sowa ◽  
J. M. MacLaren ◽  
X. -G. Zhang ◽  
A. Gonis

ABSTRACTWe describe a technique for computing self-consistent electronic structures and total energies of planar defects, such as interfaces, which are embedded in an otherwise perfectcrystal. As in the Layer Korringa-Kohn-Rostoker approach, the solid is treated as a set of coupled layers of atoms, using Bloch's theorem to take advantage of the two-dimensional periodicity of the individual layers. The layers are coupled using the techniques of the Real-Space Multiple-Scattering Theory, avoiding artificial slab or supercell boundary conditions. A total-energy calculation on a Cu crystal, which has been split apart at a (111) plane, is used to illustrate the method.


1964 ◽  
Vol 135 (4A) ◽  
pp. A969-A973 ◽  
Author(s):  
E. C. Snow ◽  
J. M. Canfield ◽  
J. T. Waber

1997 ◽  
Vol 494 ◽  
Author(s):  
G. Santi ◽  
T. Jarlborg

ABSTRACTWe study some compounds of the perovskite (or pseudo-cubic perovskite) series AMO3, where M is a transition metal and A is Ca, Sr, or Nd, by LSDA self-consistent electronic structure calculations with the LMTO method. Transport and magnetic properties, as well as Fermi surfaces are calculated. These materials exhibit sharp density of states features in the vicinity of the Fermi level that strongly affect their transport and magnetic properties and make them very sensitive to structural deformation and stoichiometry. Calculated total energies are very close for anti-ferromagnetic and ferromagnetic solutions. This explains qualitatively the magnetoresistive anomalies shown by this family of compounds.


2021 ◽  
Vol 155 (4) ◽  
pp. 044109
Author(s):  
Emmanuel Giner ◽  
Diata Traore ◽  
Barthélemy Pradines ◽  
Julien Toulouse

1990 ◽  
Vol 193 ◽  
Author(s):  
Jeremy Broughton ◽  
Mark Pederson ◽  
Dimitrios Papaconstantopoulos ◽  
David Singh

ABSTRACTA self-consistent non-orthogonal semi-empirical tight binding Hamiltonian is proposed for GaAs, or any sp system, which is simple, reliable, transferable, accurate and fast to evaluate. Matrix elements are functions of charges, distances between atoms and simple cosines of angles between s and p-electron densities and interatomic vectors which maintain the simplicity of Slater-Koster parameterizations. The tight binding scheme is fit against a large data base of local density functional derived total energies for systems of differing coordination and geometry. The Hamiltonian fulfills the correct Virial constraint, invokes the physically correct relationship between overlap and kinetic energy matrix elements and defines charges via Mulliken or Löwdin schemes. Such Hamiltonians will allow the reliable simulation of statistical mechanically interesting systems of order hundred or more atoms over physically useful periods of time of order tens to hundreds of thousands of time steps within not unreasonable supercomputer budgets.


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