Spin dynamics and magnetic frustration effects in La1−xSrxCoO3 (0

2005 ◽  
Vol 97 (10) ◽  
pp. 10A509 ◽  
Author(s):  
Nguyen Van Khiem ◽  
Nguyen Xuan Phuc ◽  
The-Long Phan ◽  
Seong-Cho Yu ◽  
Manh-Huong Phan
2003 ◽  
Vol 93 (10) ◽  
pp. 8200-8202 ◽  
Author(s):  
Manh-Huong Phan ◽  
V. Srinivas ◽  
Seong-Cho Yu ◽  
Nam Hwi Hur

2005 ◽  
Vol 290-291 ◽  
pp. 1005-1008 ◽  
Author(s):  
T.L. Phan ◽  
M.H. Phan ◽  
L.V. Bau ◽  
N.X. Phuc ◽  
S.C. Yu

2013 ◽  
Vol 62 (12) ◽  
pp. 1914-1918 ◽  
Author(s):  
Hikaru Takeda ◽  
Yasuhiro Shimizu ◽  
Masayuki Itoh ◽  
Hiroya Sakurai ◽  
Eiji Takayama-Muromachi

2011 ◽  
Vol 273 ◽  
pp. 012036 ◽  
Author(s):  
Yu Jiang ◽  
C H Booth ◽  
P H Tobash ◽  
K Gofryk ◽  
M A Torrez ◽  
...  

2020 ◽  
Author(s):  
Sourav Marik ◽  
Deepak Singh ◽  
Bruno Gonano ◽  
Fabien Veillon ◽  
Denis Pelloquin ◽  
...  

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

In the previous chapters we described the basic principles of density functional theory, gave examples of how accurate it is to describe static magnetic properties in general, and derived from this basis the master equation for atomistic spin-dynamics; the SLL (or SLLG) equation. However, one term was not described in these chapters, namely the damping parameter. This parameter is a crucial one in the SLL (or SLLG) equation, since it allows for energy and angular momentum to dissipate from the simulation cell. The damping parameter can be evaluated from density functional theory, and the Kohn-Sham equation, and it is possible to determine its value experimentally. This chapter covers in detail the theoretical aspects of how to calculate theoretically the damping parameter. Chapter 8 is focused, among other things, on the experimental detection of the damping, using ferromagnetic resonance.


Author(s):  
M. M. Glazov

In this chapter, some prospects in the field of electron and nuclear spin dynamics are outlined. Particular emphasis is put ona situation where the hyperfine interaction is so strong that it leads to a qualitative rearrangement of the energy spectrum resulting in the coherent excitation transfer between the electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized, for example in the case of deep impurity centers in semiconductors or in isotopically purified systems. We also discuss the effect of the nuclear spin polaron, that is ordered state, formation at low enough temperatures of nuclear spins, where the orientation of the carrier spin results in alignment of the spins of nucleus interacting with the electron or hole.


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