scholarly journals Exchange biasing by Ir19Mn81: Dependence on temperature, microstructure and antiferromagnetic layer thickness

2000 ◽  
Vol 88 (2) ◽  
pp. 975-982 ◽  
Author(s):  
J. van Driel ◽  
F. R. de Boer ◽  
K.-M. H. Lenssen ◽  
R. Coehoorn
1996 ◽  
Vol 79 (8) ◽  
pp. 5103 ◽  
Author(s):  
P. J. van der Zaag ◽  
A. R. Ball ◽  
L. F. Feiner ◽  
R. M. Wolf ◽  
P. A. A. van der Heijden

2007 ◽  
Vol 7 (1) ◽  
pp. 356-361 ◽  
Author(s):  
Xiaowei Teng ◽  
Hong Yang

This paper presents a synthesis of magnetic nanoparticles of samarium cobalt alloys and the use of iron oxide as a coating layer to prevent the rapid oxidation of as-made Sm–Co nanoparticles. The colloidal nanoparticles of Sm–Co alloys were made in octyl ether using samarium acetylacetonate and dicobalt octacarbonyl as precursors in a mixture of 1,2-hexadecanediol, oleic acid, and trioctylphosphine oxide (TOPO). Such Sm–Co nanoparticle could be readily oxidized by air and formed a CoO antiferromagnetic layer. Exchange biasing was observed for the surface oxidized nanoparticles. In situ thermal decomposition of iron pentacarbonyl was used to create iron oxide shells on the Sm–Co nanoparticles. The iron oxide shell could prevent Sm–Co nanoparticles from rapid oxidation upon the exposure to air at ambient conditions.


2002 ◽  
Vol 746 ◽  
Author(s):  
Markus Kirschner ◽  
Dieter Suess ◽  
Thomas Schrefl ◽  
Josef Fidler

ABSTRACTExchange bias and training effect are simulated for IrMn/NiFe bilayers. As a function of the thickness of the antiferromagnet the bias field shows a maximum for a thickness of 22 nm. For decreasing antiferromagnetic thickness the domain wall energy approaches zero. For large thicknesses the high anisotropy energy hinders switching of the antiferromagnetic grains resulting in weak bias. Starting from the field cooled state as initial configuration a bias field of about 8 mT is obtained assuming a antiferromagnetic layer thickness of 20 nm, a ferromagnetic layer thickness of 10 nm, and a grain size of 10 nm. The next hysteresis cycle shows a reduction of the bias field by about 65%. Exchange bias and training effect in fully compensated antiferromagnet/ferromagnet bilayers are explained with a simple micromagnetic model. The model assumes no defects except for grain boundaries, and coupling is due to spin flop at a perfect interface. The simulations show that a weak exchange interaction between randomly oriented antiferromagnetic grains and spin flop coupling at a perfectly compensated interface are sufficient to support exchange bias.


2008 ◽  
Vol 77 (4) ◽  
pp. 044602 ◽  
Author(s):  
Chiharu Mitsumata ◽  
Akimasa Sakuma ◽  
Kazuaki Fukamichi ◽  
Masakiyo Tsunoda ◽  
Migaku Takahashi

2010 ◽  
Vol 81 (22) ◽  
Author(s):  
Hyeok-Cheol Choi ◽  
Chun-Yeol You ◽  
Ki-Yeon Kim ◽  
Jeong-Soo Lee ◽  
Je-Ho Shim ◽  
...  

Author(s):  
Daniel J Adams ◽  
Dorin Cimpoesu ◽  
Simeon P Benit ◽  
Danielle Maurin ◽  
Paula Kern ◽  
...  

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