Experimental determination of spin-transfer torque nonadiabaticity parameter and spin polarization in permalloy

2009 ◽  
Vol 79 (9) ◽  
Author(s):  
S. Lepadatu ◽  
M. C. Hickey ◽  
A. Potenza ◽  
H. Marchetto ◽  
T. R. Charlton ◽  
...  
2016 ◽  
Vol 7 (1) ◽  
Author(s):  
Sunjae Chung ◽  
Anders Eklund ◽  
Ezio Iacocca ◽  
Seyed Majid Mohseni ◽  
Sohrab R. Sani ◽  
...  

Abstract Static and dynamic magnetic solitons play a critical role in applied nanomagnetism. Magnetic droplets, a type of non-topological dissipative soliton, can be nucleated and sustained in nanocontact spin-torque oscillators with perpendicular magnetic anisotropy free layers. Here, we perform a detailed experimental determination of the full droplet nucleation boundary in the current–field plane for a wide range of nanocontact sizes and demonstrate its excellent agreement with an analytical expression originating from a stability analysis. Our results reconcile recent contradicting reports of the field dependence of the droplet nucleation. Furthermore, our analytical model both highlights the relation between the fixed layer material and the droplet nucleation current magnitude, and provides an accurate method to experimentally determine the spin transfer torque asymmetry of each device.


Author(s):  
K. Takanashi ◽  
Y. Sakuraba

This chapter explains how the exchange splitting between up- and down-spin bands in ferromagnets unexceptionally generates spin-polarized electronic states at the Fermi energy. The quantity of spin polarization P in ferromagnets is one of the important parameters for application in spintronics, since a ferromagnet having a higher P is able to generate larger various spin-dependent effects such as the magnetoresistance effect, spin transfer torque, spin accumulation, and so on. However, the spin polarizations of general 3d transition metals or alloys generally limit the size of spin-dependent effects. Thus,“‘half-metals” attract much interest as an ideal source of spin current and spin-dependent scattering because they possess perfectly spin-polarized conduction electrons due to the energy band gap in either the up- or down-spin channel at the Fermi level.


2019 ◽  
Vol 52 (50) ◽  
pp. 505005 ◽  
Author(s):  
N Perrissin ◽  
N Caçoilo ◽  
G Gregoire ◽  
S Lequeux ◽  
L Tillie ◽  
...  

2014 ◽  
Vol 89 (2) ◽  
Author(s):  
J.-Y. Chauleau ◽  
H. G. Bauer ◽  
H. S. Körner ◽  
J. Stigloher ◽  
M. Härtinger ◽  
...  

1999 ◽  
Vol 96 (6) ◽  
pp. 1111-1116 ◽  
Author(s):  
E. Falcon ◽  
S. Fauve ◽  
C. Laroche

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