Fourier analysis of exchange biased Ni80Fe20/Fe50Mn50/Ni80Fe20 trilayers

Citation
S. Maat et al., Fourier analysis of exchange biased Ni80Fe20/Fe50Mn50/Ni80Fe20 trilayers, PHYS REV B, 60(14), 1999, pp. 10252-10258
Citations number
28
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B-CONDENSED MATTER
ISSN journal
01631829 → ACNP
Volume
60
Issue
14
Year of publication
1999
Pages
10252 - 10258
Database
ISI
SICI code
0163-1829(19991001)60:14<10252:FAOEBN>2.0.ZU;2-9
Abstract
Hysteresis loops of polycrystalline and single-crystal exchange biased Ni80 Fe20 (Permalloy)/ Fe50Mn50/Ni80Fe20 (Permalloy) trilayers were measured as a function of Fe50Mn50 layer thickness with the longitudinal Kerr effect. T he variation of the macroscopic pinning field H-p and the coercivity H-c wa s observed over a full 360 degrees in plane rotation and Fourier analyzed. The magnetization behavior of both Permalloy layers of the polycrystalline samples was analyzed, and it was found that the pinning field of the bottom layer is always greater than for the top layer, while the situation is rev ersed for the coercivity due to defects incorporated in the antiferromagnet ic layer. The single-crystal samples were prepared on epitaxially grown Cu( 111) on Si(110), and the magnetization behavior of the top Permalloy layer was studied. In contrast to the polycrystalline samples, the coercivities p eak very sharply at the easy axis, which manifests itself in large higher-o rder Fourier coefficients. Coercivities and loop shifts show a strong linea r dependence on the antiferromagnetic layer thickness. The relation of the biasing direction to the crystal axes had no influence on H-c acid H-p. Thi s behavior is attributed to complete strain relief through the buffer layer and better crystalline growth of the trilayer as compared to the polycryst alline samples. Examination of the results with a Ginzburg-Landau energy fu nctional verified that the Fourier coefficients obey necessary conditions t o achieve energetic stability together with spontaneous magnetization. The energy functional was used to model the angular dependence of the loop shif t.