Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
Noncontact Atomic Force Microscopy - Yale School of Engineering ...
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P.II-35<br />
Enhancement <strong>of</strong> the Exchange-bias Effect based on Quantitative<br />
Magnetic <strong>Force</strong> <strong>Microscopy</strong> Results.<br />
N. Pilet 1 , M.A. Marioni 1 , S. Romer 1 , N. Joshi 2 , S. Özer 2 and H.J. Hug, 1,2<br />
1 Empa, Swiss Federal Institute for Materials Testing and Research, CH-8600 Duebendorf, Switzerland,<br />
2 Department <strong>of</strong> Physics, University <strong>of</strong> Basel, Klingelbergstrasse 82, CH-4056 Basel, Switzerland<br />
Exchange biasing (EB) causes a lateral shift <strong>of</strong> the magnetization vs. field curve in<br />
antiferromagnetic-ferromagnetic (AF-F) thin-film structures. It is largely believed that<br />
EB arises from linking the magnetization <strong>of</strong> the F to that <strong>of</strong> (pinned) uncompensated<br />
spins (UCS) in the AF. In the present work we are able to measure the local density <strong>of</strong><br />
UCS on the scale <strong>of</strong> 20 nm, using quantitative magnetic force microscopy (qMFM). With<br />
quantitative results at this lateral resolution, it becomes possible to resolve and measure<br />
the UCS underneath each F domain at scales comparable to the grain size. The average<br />
density <strong>of</strong> UCS around 20% <strong>of</strong> that expected for a full monolayer <strong>of</strong> spins is considerably<br />
higher than expected from the measured exchange field and local values may reach<br />
100%. We found that UCSs coupling antiparallel to the F magnetization stabilize its<br />
orientation, i.e. they are biasing [1,2]. Locally, UCS oriented parallel to the F<br />
magnetization were found. These have an antibiasing effect and are hence expected to<br />
weaken the exchange field. We hypothesized that such anti-biasing arises from<br />
conflicting exchange interaction between the F-layer and AF-grains, and between AFgrains<br />
themselves. Exchange-bias systems grown with suppressed inter-granular coupling<br />
in the AF-layer proved our hypothesis to be correct. These systems showed an exchangebias<br />
effect enhanced by 20%. High resolution MFM revealed a more homogenous pattern<br />
<strong>of</strong> UCS with a correspondingly higher density. The evolution <strong>of</strong> the F-domains in an<br />
applied field was strikingly different.<br />
Figure 1: . (A) UCS density calculated from measured MFM data and the instrument calibration<br />
function. Positive UCS (i.e. parallel to the cooling field) are colored yellow, negative UCS red.<br />
(B) UCS with overlayed contours <strong>of</strong> the F domains at H = 0; (C) Idem for H = 200mT. With few<br />
exceptions (such as pointed out by the arrows) the UCS align antiparallel to the domain<br />
magnetization at H=0.<br />
[1] I. Schmid, P. Kappenberger, O. Hellwig, M. Carey, E. Fullerton and H. J. Hug, EPL 81 (2008) 17001<br />
[2] I. Schmid, M. Marioni et al. submitted.<br />
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