Ab initio non-relativistic spin dynamics

2014 ◽  
Vol 141 (21) ◽  
pp. 214111 ◽  
Author(s):  
Feizhi Ding ◽  
Joshua J. Goings ◽  
Michael J. Frisch ◽  
Xiaosong Li
2005 ◽  
Vol 32 (1) ◽  
pp. 118-122 ◽  
Author(s):  
M. Fähnle ◽  
R. Drautz ◽  
R. Singer ◽  
D. Steiauf ◽  
D.V. Berkov

2021 ◽  
Vol 104 (2) ◽  
Author(s):  
J. Wang ◽  
X. B. Li ◽  
L. F. Gan ◽  
C. T. Zhou ◽  
S. P. Zhu ◽  
...  

2020 ◽  
Vol 102 (21) ◽  
Author(s):  
Simon Streib ◽  
Vladislav Borisov ◽  
Manuel Pereiro ◽  
Anders Bergman ◽  
Erik Sjöqvist ◽  
...  

2018 ◽  
Vol 6 (35) ◽  
pp. 16983-16991 ◽  
Author(s):  
Jeongjae Lee ◽  
Bartomeu Monserrat ◽  
Ieuan D. Seymour ◽  
Zigeng Liu ◽  
Siân E. Dutton ◽  
...  

We show that vacancy creation and relativistic spin–orbit coupling play a crucial role in promoting fast Mg-ion conduction of Mg3Bi2.


2021 ◽  
Vol 104 (18) ◽  
Author(s):  
Junqing Xu ◽  
Adela Habib ◽  
Ravishankar Sundararaman ◽  
Yuan Ping
Keyword(s):  

2011 ◽  
Vol 79 (10) ◽  
pp. 1064-1067 ◽  
Author(s):  
Krzysztof Rębilas

Author(s):  
Olle Eriksson ◽  
Anders Bergman ◽  
Lars Bergqvist ◽  
Johan Hellsvik

In Chapter 4 we presented a microscopic mechanism behind the LL equation and its connection to ab-initio results, such as that provided by density functional theory. All the analysis of Chapter 4 was done by considering a temperature T=0 K. Since most magnetic phenomena of interest are observed at finite temperature, it is important to generalize the analysis presented above to incorporate effects of finite temperature. In the discussion of Eqn. 4.1 it was mentioned briefly that finite temperature effects are incorporated in the stochastic field. Details of the coupling between temperature and the stochastic field, is the main topic of this chapter.


Author(s):  
Xudong Weng ◽  
O.F. Sankey ◽  
Peter Rez

Single electron band structure techniques have been applied successfully to the interpretation of the near edge structures of metals and other materials. Among various band theories, the linear combination of atomic orbital (LCAO) method is especially simple and interpretable. The commonly used empirical LCAO method is mainly an interpolation method, where the energies and wave functions of atomic orbitals are adjusted in order to fit experimental or more accurately determined electron states. To achieve better accuracy, the size of calculation has to be expanded, for example, to include excited states and more-distant-neighboring atoms. This tends to sacrifice the simplicity and interpretability of the method.In this paper. we adopt an ab initio scheme which incorporates the conceptual advantage of the LCAO method with the accuracy of ab initio pseudopotential calculations. The so called pscudo-atomic-orbitals (PAO's), computed from a free atom within the local-density approximation and the pseudopotential approximation, are used as the basis of expansion, replacing the usually very large set of plane waves in the conventional pseudopotential method. These PAO's however, do not consist of a rigorously complete set of orthonormal states.


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