scholarly journals Spin dynamics in the stripe-ordered buckled honeycomb lattice antiferromagnet Ba2NiTeO6

2017 ◽  
Vol 96 (10) ◽  
Author(s):  
Shinichiro Asai ◽  
Minoru Soda ◽  
Kazuhiro Kasatani ◽  
Toshio Ono ◽  
V. Ovidiu Garlea ◽  
...  
2021 ◽  
Vol 103 (18) ◽  
Author(s):  
Feng Ye ◽  
Zachary Morgan ◽  
Wei Tian ◽  
Songxue Chi ◽  
Xiaoping Wang ◽  
...  

2017 ◽  
Vol 96 (24) ◽  
Author(s):  
A. N. Ponomaryov ◽  
E. Schulze ◽  
J. Wosnitza ◽  
P. Lampen-Kelley ◽  
A. Banerjee ◽  
...  

2011 ◽  
Vol 80 (2) ◽  
pp. 023705 ◽  
Author(s):  
Susumu Okubo ◽  
Hideo Wada ◽  
Hitoshi Ohta ◽  
Takahiro Tomita ◽  
Masashi Fujisawa ◽  
...  

2020 ◽  
Vol 16 (4) ◽  
pp. 595-607 ◽  
Author(s):  
Mu Wen Chuan ◽  
Kien Liong Wong ◽  
Afiq Hamzah ◽  
Shahrizal Rusli ◽  
Nurul Ezaila Alias ◽  
...  

Catalysed by the success of mechanical exfoliated free-standing graphene, two dimensional (2D) semiconductor materials are successively an active area of research. Silicene is a monolayer of silicon (Si) atoms with a low-buckled honeycomb lattice possessing a Dirac cone and massless fermions in the band structure. Another advantage of silicene is its compatibility with the Silicon wafer fabrication technology. To effectively apply this 2D material in the semiconductor industry, it is important to carry out theoretical studies before proceeding to the next step. In this paper, an overview of silicene and silicene nanoribbons (SiNRs) is described. After that, the theoretical studies to engineer the bandgap of silicene are reviewed. Recent theoretical advancement on the applications of silicene for various field-effect transistor (FET) structures is also discussed. Theoretical studies of silicene have shown promising results for their application as FETs and the efforts to study the performance of bandgap-engineered silicene FET should continue to improve the device performance.


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.


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