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Keywords
(14)
Cross Section
Domain Structure
Exchange Bias
Grain Size
Hysteresis Loop
Magnetic Force Microscopy
Magnetic Properties
Magnetization Reversal
Room Temperature
Scattered Data
Specular Reflection
Weak Dependence
X Rays
Domain Wall
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Nonuniform and sequential magnetization reversal via domain structure formation formultilayered system with grain size induced enhanced exchangebias
Nonuniform and sequential magnetization reversal via domain structure formation formultilayered system with grain size induced enhanced exchangebias,1
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Nonuniform and sequential magnetization reversal via domain structure formation formultilayered system with grain size induced enhanced exchangebias
(
Citations: 1
)
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A. Paul
,
E. Kentzinger
,
U. Rücker
,
D. E. Bürgler
,
P. Grünberg
We report on the
magnetization reversal
in series of exchange-biased multilayers NiFe(10.0 nm)/[ Ir20Mn80(6.0 nm)/Co80Fe20(3.0 nm)] N studied by
specular reflection
and off-specular scattering of polarized neutrons. All specimens are sputtered and post-annealed at 530 K (i.e. above the IrMn Néel temperature of 520 K) in Ar atmosphere before cooling to
room temperature
in the presence of a field of 130 Oe which induces the unidirectional anisotropy. We find HEB is dependent upon the number of bilayers N as it gradually increases from 0.33 kOe for N=1 to a considerably higher value of upto ˜0.9 kOe for N=10. X-ray specular and diffuse scattering data reveal no significant variation of the lateral correlation length and only a
weak dependence
of the vertical rms interface roughness on N. Atomic and magnetic force microscopy, however, show a strong reduction of the
grain size
accompanied by distinct changes of the ferromagnetic domain structure. The enhancement of the
exchange bias
effect is presumably related to the shrinking of the related domain size in the antiferromagnet due to the structural evolution in the multilayers. Polarized neutron reflectometry (PNR) measurements are done at different applied fields sweeping both branches of the hysteresis loop. The spin-flip (SF)
cross section
of both the N=10 and 3 samples show diffusely scattered intensity appears gradually as the field approaches HEB and is most intense where the net magnetization vanishes. The disappearance of diffuse scattering in saturation indicates that the off-specular intensity is related to the reversal process. The reversal proceeds sequentially starting with the bottom (top) CoFe layer for decreasing (increasing) field and is related to the evolution of the
grain size
along the stack. The reversal of each CoFe layer is for both field branches due to
domain wall
motion. Thus as a main result, we observe a sequential and symmetric
magnetization reversal
in exchange-biased multilayers. The concomitant in-plane magnetization fluctuations revealed by off-specular spin-flip scattering indicate a more complex reversal mechanism than hitherto considered. Moreover, although the
grain size
decreases from N=3 to 10 by a factor of about four the reversal mechanism remains similar.
Journal:
European Physical Journal B - EUR PHYS J B
, vol. 45, no. 2, pp. 249-260, 2005
DOI:
10.1140/epjb/e2005-00056-0
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References
(28)
Exchange bias
(
Citations: 239
)
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,
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Journal:
Journal of Magnetism and Magnetic Materials - J MAGN MAGN MATER
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(
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(
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Journal:
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(
Citations: 1
)
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Physical Review B - PHYS REV B
, vol. 62, no. 17, pp. 11340-11343, 2000
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Citations
(1)
und J. Schmitt ( 1969): "Crystal Field In Dysprosium Garnets" Physical Review 184(2): 285ff. Grünberg, P
E. Orlich
,
S. Hüfner