Magnetization dynamics in interlayer exchange-coupled in-plane/out-of-plane anisotropy bilayers

2009 ◽  
Vol 79 (18) ◽  
Author(s):  
N. Vukadinovic ◽  
J. Ben Youssef ◽  
V. Castel ◽  
M. Labrune
2009 ◽  
Vol 94 (10) ◽  
pp. 102501 ◽  
Author(s):  
G. Malinowski ◽  
K. C. Kuiper ◽  
R. Lavrijsen ◽  
H. J. M. Swagten ◽  
B. Koopmans

2021 ◽  
pp. 160249
Author(s):  
Garima Vashisht ◽  
Utkarsh Shashank ◽  
Surbhi Gupta ◽  
Rohit Medwal ◽  
C.L. Dong ◽  
...  

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Roxana-Alina One ◽  
Hélène Béa ◽  
Sever Mican ◽  
Marius Joldos ◽  
Pedro Brandão Veiga ◽  
...  

AbstractThe voltage controlled magnetic anisotropy (VCMA) becomes a subject of major interest for spintronics due to its promising potential outcome: fast magnetization manipulation in magnetoresistive random access memories with enhanced storage density and very low power consumption. Using a macrospin approach, we carried out a thorough analysis of the role of the VCMA on the magnetization dynamics of nanostructures with out-of-plane magnetic anisotropy. Diagrams of the magnetization switching have been computed depending on the material and experiment parameters (surface anisotropy, Gilbert damping, duration/amplitude of electric and magnetic field pulses) thus allowing predictive sets of parameters for optimum switching experiments. Two characteristic times of the trajectory of the magnetization were analyzed analytically and numerically setting a lower limit for the duration of the pulses. An interesting switching regime has been identified where the precessional reversal of magnetization does not depend on the voltage pulse duration. This represents a promising path for the magnetization control by VCMA with enhanced versatility.


1999 ◽  
Vol 12 (10) ◽  
pp. 690-693 ◽  
Author(s):  
S Kokkaliaris ◽  
K Deligiannis ◽  
M Oussena ◽  
A A Zhukov ◽  
P A J de Groot ◽  
...  

2013 ◽  
Vol 1517 ◽  
Author(s):  
Petar Popčević ◽  
Ante Bilušić ◽  
Kristijan Velebit ◽  
Ana Smontara

ABSTRACTTransport properties (thermal conductivity, electrical resistivity and thermopower) of decagonal quasicrystal d-AlCoNi, and approximant phases Y-AlCoNi, o-Al13Co4, m-Al13Fe4, m-Al13(Fe,Ni)4 and T-AlMnFe have been reviewed. Among all presented alloys the stacking direction (periodic for decagonal quasicrystals) is the most conductive one for the charge and heat transport, and the in/out-of-plane anisotropy is much larger than the in-plane anisotropy. There is a strong relationship between periodicity length along stacking direction and anisotropy of transport properties in both quasicrystals and their approximants suggesting a decrease of the anisotropy with increasing number of stacking layers.


2020 ◽  
Vol 102 (17) ◽  
Author(s):  
Andrey O. Leonov ◽  
Ivan M. Tambovtcev ◽  
Igor S. Lobanov ◽  
Valery M. Uzdin

SPIN ◽  
2019 ◽  
Vol 09 (03) ◽  
pp. 1950008
Author(s):  
HaoHsuan Chen ◽  
Lang Zeng ◽  
ChingMing Lee ◽  
Weisheng Zhao

Spin-torque nano-oscillators (STNOs) have become one of the emerging and novel microwave devices with the high performance and tunability of GHz range frequency. The nanopillar structure with an out-of-plane (OP) spin polarizer and an in-plane (IP) magnetized free layer (FL) has been considered as a good candidate for the STNOs. Using the local rotational coordinate transformation, a nonstationary process describing magnetization dynamics in the laboratory frame is therefore transformed into a stationary one in the rotating frame. In this way, the state phase diagram of this type of STNOs is well established as a function of an applied current and external field, which is also evidenced by the macrospin simulations. Also, we show that the frequency tunability of the STNOs through electrical current can be well elevated by applying a static magnetic field anti-parallel to the spin-polarizer vector.


2003 ◽  
Vol 67 (2) ◽  
Author(s):  
M. Ciria ◽  
J. I. Arnaudas ◽  
L. Benito ◽  
C. de la Fuente ◽  
A. del Moral ◽  
...  

2007 ◽  
Vol 101 (9) ◽  
pp. 09C101 ◽  
Author(s):  
T. Martin ◽  
M. Belmeguenai ◽  
M. Maier ◽  
K. Perzlmaier ◽  
G. Bayreuther

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