2014
DOI: 10.1063/1.4870291
|View full text |Cite
|
Sign up to set email alerts
|

Modelling current-induced magnetization switching in Heusler alloy Co2FeAl-based spin-valve nanopillar

Abstract: We investigated the current-induced magnetization switching in a Heusler alloy Co 2 FeAl-based spin-valve nanopillar by using micromagnetic simulations. We demonstrated that the elimination of the intermediate state is originally resulted from the decease of effective magnetic anisotropy constant. The magnetization switching can be achieved at a small current density of 1.0 Â 10 4 A/cm 2 by increasing the demagnetization factors of x and y axes. Based on our simulation, we found magnetic anisotropy and demagne… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
4
0

Year Published

2014
2014
2023
2023

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 9 publications
(4 citation statements)
references
References 35 publications
0
4
0
Order By: Relevance
“…The dynamics of magnetization was investigated by numerically solving the time-dependent LLGS equation using the Gauss-Seidel projection method and the semi-implicit Fourier spectral method. 44,45 The samples were discretized in computational cells of 2 Â 2 Â 2 nm 3 , and the total size is 80 Â 80 Â 20 nm 3 . 46 Figure 2…”
mentioning
confidence: 99%
“…The dynamics of magnetization was investigated by numerically solving the time-dependent LLGS equation using the Gauss-Seidel projection method and the semi-implicit Fourier spectral method. 44,45 The samples were discretized in computational cells of 2 Â 2 Â 2 nm 3 , and the total size is 80 Â 80 Â 20 nm 3 . 46 Figure 2…”
mentioning
confidence: 99%
“…The dynamics of magnetization is investigated by numerically solving the timedependent LLGS equation using the Gauss-Seidel projection method with a constant time step ∆t= 0.0268858 ps. [36][37][38] We adopted the following magnetic parameters, magnetocrystalline anisotropy constant K 1 =3.0×10 3 J/m 3 , and K 2 =0, 39 exchange constant A=2.0×10 -11 J/m, 40 saturation magnetization M s =8.0×10 5 A/m. 41 Other parameters are Gilbert damping parameter α=0.008, 14 spin polarization factor η=0.56, 42,43 electron gyromagnetic ratio γ=2.3245×10 5 For clarify, the PSD of y axis shifts up with 0.5 each curve with the increase of external stress.…”
Section: Methodsmentioning
confidence: 99%
“…Moreover, they generally display a perpendicular anisotropy which has been experimentally carried out for certain Heusler alloys [15]. Thanks to these characteristics, recent experiences and simulations demonstrated the ability to get the magnetization switching from a low current density of about 10 6 -10 4 A/cm 2 [7,[16][17][18][19].…”
Section: Introductionmentioning
confidence: 94%