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Effect of ultra-thin Cu underlayer on the magnetic properties of Ni80Fe50 / Fe50Mn50 films

Published online by Cambridge University Press:  10 February 2011

C. Liu
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
L. Shen
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
H. Jiang
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
D. Yang
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
G. Wu
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
C. Alexander
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
G. J. Mankey
Affiliation:
Center for Materials for Information Technology, University of Alabama, Box 870209, Tuscaloosa, AL 35487-0209, [email protected]
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Abstract

The Ni80Fe20/Fe50Mn50,thin film system exhibits exchange bias behavior. Here a systematic study of the effect of atomic-scale thin film roughness on coercivity and exchange bias is presented. Cu (t) / Ta (100 Å) / Ni80Fe20 (100 Å) / Fe50Mno50 (200 Å) / Ta (200 Å) with variable thickness, t, of the Cu underlayer were DC sputtered on Si (100) substrates. The Cu underlayer defines the initial roughness that is transferred to the film material since the film grows conformal to the initial morphology. Atomic Force Microscopy and X-ray diffraction were used to study the morphology and texture of the films. Morphological characterization is then correlated with magnetometer measurements. Atomic Force Microscopy shows that the root mean square value of the film roughness exhibits a maximum of 2.5 Å at t = 2.4 Å. X-ray diffraction spectra show the films are polycrystalline with fcc (111) texture and the Fe50Mn50 (111) peak intensity decreases monotonically with increasing Cu thickness, t. Without a Cu underlayer, the values of the coercivity and loop shift are, Hc = 12 Oe and Hp = 56 Oe, respectively. Both the coercivity and loop shift change with Cu underlayer thickness. The coercivity reaches a maximum value of Hc= 36 Oe at t = 4 Å. The loop shift exhibits an initial increase with t, reaches a maximum value of HP = 107 Oe at t = 2.4 Å, followed by a decrease with greater Cu thickness. These results show that a tiny increase in the film roughness has a huge effect on the exchange bias magnitude.

Type
Research Article
Copyright
Copyright © Materials Research Society 1999

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References

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