Ultrafast Spin Dynamics in the Iron Borate Easy-Plane Weak Ferromagnet

2020 ◽  
Vol 131 (1) ◽  
pp. 130-138
Author(s):  
A. K. Zvezdin ◽  
A. V. Kimel ◽  
D. I. Plokhov ◽  
K. A. Zvezdin
1992 ◽  
Vol 104-107 ◽  
pp. 1067-1068 ◽  
Author(s):  
H. Grille ◽  
G. Kamieniarz ◽  
R.W. Gerling

1986 ◽  
Vol 54-57 ◽  
pp. 673-674 ◽  
Author(s):  
M.T. Hutchings ◽  
P. Day ◽  
E. Janke ◽  
R. Pynn

1993 ◽  
Vol 48 (17) ◽  
pp. 12698-12703 ◽  
Author(s):  
A. S. T. Pires ◽  
M. E. Gouvêa

1993 ◽  
Vol 505 (3) ◽  
pp. 308-319 ◽  
Author(s):  
A. R. Völkel ◽  
F. G. Mertens ◽  
A. R. Bishop ◽  
G. M. Wysin

1971 ◽  
Vol 32 (C1) ◽  
pp. C1-1149-C1-1150
Author(s):  
V. A. SANINA ◽  
E. I. GOLOVENCHITS ◽  
T. A. FOMINA ◽  
A. G. GUREVICH

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.


Sign in / Sign up

Export Citation Format

Share Document