scholarly journals Magnetic layer thickness dependence of the interlayer exchange coupling in (001) Co/Cu/Co

1994 ◽  
Vol 76 (10) ◽  
pp. 7081-7083 ◽  
Author(s):  
P. J. H. Bloemen ◽  
M. T. H. van de Vorst ◽  
M. T. Johnson ◽  
R. Coehoorn ◽  
W. J. M. de Jonge
Keyword(s):  
Layer Thickness ◽  
Exchange Coupling ◽  
Magnetic Layer ◽  
Thickness Dependence ◽  
Interlayer Exchange Coupling ◽  
Interlayer Exchange

scholarly journals Magnetic layer thickness dependence of the interlayer exchange coupling in (001) Co/Cu/Co

1994 ◽  
Vol 72 (5) ◽  
pp. 764-767 ◽  
Author(s):  
P. J. H. Bloemen ◽  
M. T. Johnson ◽  
M. T. H. van de Vorst ◽  
R. Coehoorn ◽  
J. J. de Vries ◽  
...  
Keyword(s):  
Layer Thickness ◽  
Exchange Coupling ◽  
Magnetic Layer ◽  
Thickness Dependence ◽  
Interlayer Exchange Coupling ◽  
Interlayer Exchange

MAGNETIC LAYER THICKNESS DEPENDENCE OF THE INTERLAYER EXCHANGE COUPLING

1995 ◽  
Vol 09 (01) ◽  
pp. 1-25 ◽  
Author(s):  
P. J. H. BLOEMEN ◽  
M. T. H. VAN DE VORST ◽  
W. J. M. DE JONGE ◽  
M. T. JOHNSON ◽  
R. COEHOORN
Keyword(s):  
Electronic Properties ◽  
Layer Thickness ◽  
Exchange Coupling ◽  
Recent Progress ◽  
Magnetic Layer ◽  
Thickness Dependence ◽  
Interlayer Exchange Coupling ◽  
Fermi Surfaces ◽  
Interlayer Exchange

Recent progress in the research on interlayer exchange coupling, focusing on the effect of the magnetic layer, is reviewed. Several theoretical works have shown that the exchange coupling does not just involve an interaction localized at the interfaces, but the electronic properties of the sandwich as a whole. The important prediction that the strength of the exchange coupling should oscillate as a function of the magnetic layer thickness has been confirmed recently for the Co/Cu(100) and the Fe/Cr(100) system. The oscillation periods are strongly believed to be related to wave vectors that span extremal parts of the spin-resolved Fermi surfaces of the ferromagnets.

Oscillatory Interlayer Exchange Coupling with the Cu Cap Layer Thickness in Co/Cu/Co/Cu(100)

1995 ◽  
Vol 75 (23) ◽  
pp. 4306-4309 ◽  
Author(s):  
J. J. de Vries ◽  
A. A. P. Schudelaro ◽  
R. Jungblut ◽  
P. J. H. Bloemen ◽  
A. Reinders ◽  
...  
Keyword(s):  
Layer Thickness ◽  
Exchange Coupling ◽  
Interlayer Exchange Coupling ◽  
Cap Layer ◽  
Interlayer Exchange

scholarly journals MFM studies of interlayer exchange coupling in Co/Ru/Co films: Effect of Ru layer thickness

2009 ◽  
Vol 109 (8) ◽  
pp. 1040-1043 ◽  
Author(s):  
Lanping Yue ◽  
Zhen Li ◽  
Roger Kirby ◽  
David Sellmyer
Keyword(s):  
Layer Thickness ◽  
Exchange Coupling ◽  
Interlayer Exchange Coupling ◽  
Interlayer Exchange

scholarly journals Spacer-thickness dependence of interlayer exchange coupling in GaMnAs/InGaAs/GaMnAs trilayers grown on ZnCdSe buffers

2017 ◽  
Vol 253 ◽  
pp. 37-41 ◽  
Author(s):  
Kritsanu Tivakornsasithorn ◽  
Taehee Yoo ◽  
Hakjoon Lee ◽  
Seonghoon Choi ◽  
Sanghoon Lee ◽  
...  
Keyword(s):  
Exchange Coupling ◽  
Thickness Dependence ◽  
Interlayer Exchange Coupling ◽  
Spacer Thickness ◽  
Interlayer Exchange

Giant Magnetoresistance in (Ni60Co30Fe10/Cu) Trilayer Growth by Opposed Target Magnetron Sputtering

2012 ◽  
Vol 535-537 ◽  
pp. 1319-1322 ◽  
Author(s):  
Ramli ◽  
Mitra Djamal ◽  
Freddy Haryanto ◽  
Sparisoma Viridi ◽  
Khairurrijal
Keyword(s):  
Magnetron Sputtering ◽  
Layer Thickness ◽  
Exchange Coupling ◽  
Giant Magnetoresistance ◽  
Growth Parameters ◽  
Oscillatory Behavior ◽  
Interlayer Exchange Coupling ◽  
Growth Pressure ◽  
Ar Gas ◽  
Interlayer Exchange

The giant magnetoresistance thin film of (Ni60Co30Fe10/Cu) trilayer were grown onto Si (100) substrate by dc-opposed target magnetron sputtering (dc-OTMS) technique. The growth parameters are: temperature of 100 0C, applied voltage of 600 volt, flow rate of Ar gas of 100 sccm, and growth pressure of 5.2 x10-1 Torr. The effects of Cu layer thickness and NiCoFe layer thickness on giant magnetoresistance (GMR) property of (Ni60Co30Fe10/Cu) trilayer were studied. We have found that the giant magnetoresistance (GMR) ratio of the sample was varied depend on the non-magnetic (Cu) layer thickness. The variation of Cu layer thickness presents an oscillatory behavior of GMR ratio. This oscillation reflects the exchange coupling oscillations between ferromagnetic and antiferromagnetic states, which are caused by an oscillation in the sign of the interlayer exchange coupling between ferromagnetic layers. The GMR ratio is change with increasing of NiCoFe layer thickness and presents GMR ratio of 70.0 % at tNiCoFe = 62.5 nm.

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