Collinear spin-density-wave ordering in Fe Cr multilayers and wedges

被引:30
|
作者
Fishman, RS
Shi, ZP
机构
[1] Oak Ridge Natl Lab, Div Solid State, Oak Ridge, TN 37831 USA
[2] Read Rite Corp, R&D Div, Milpitas, CA 95035 USA
来源
PHYSICAL REVIEW B | 1999年 / 59卷 / 21期
关键词
D O I
10.1103/PhysRevB.59.13849
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Several recent experiments have detected a spin-density wave (SDW) within the Cr spacer of Fe/Cr multilayers and wedges. We use two simple models to predict the behavior of a collinear SDW within an Fe/Cr/Fe trilayer. Both models combine assumed boundary conditions at the Fe-Cr interfaces with the free energy of the Cr spacer. Depending on the temperature and the number N of Cr monolayers, the SDW may be either commensurate (C) or incommensurate (I) with the bcc Cr lattice. Model I assumes that the Fe-Cr interface is perfect and that the Fe-Cr interaction is antiferromagnetic. Consequently, the I SDW antinodes lie near the Fe-Cr interfaces. With increasing temperature, the Cr spacer undergoes a series of transitions between I SDW phases with different numbers n of nodes. If the I SDW has n = m nodes at T = 0, then it increases by one at each phase transition from m to m-1 to m-2 up to the C phase with n = 0 above T-IC(N). For a fixed temperature, the magnetic coupling across the Cr spacer undergoes a phase slip whenever n changes by one. In the limit N--> infinity, T-IC(N) is independent of the Fe-Cr coupling strength. We find that T-IC(infinity) is always larger than the bulk Neel transition temperature and increases with the strain on the Cr spacer. These results explain the very high IC transition temperature of about 600 K extrapolated from measurements on Fe/Cr/Fe wedges. Model II assumes that the I SDW nodes lie precisely at the Fe-Cr interfaces. This condition may be enforced by the interfacial roughness of sputtered Fe/Cr multilayers. As a result, the C phase is never stable and the transition temperature T-N(N) takes on a seesaw pattern as n greater than or equal to 2 increases with thickness. In agreement with measurements on both sputtered and epitaxially grown multilayers, model II predicts the I phase to be unstable above the bulk Neel temperature. Model II also predicts that the I SDW may undergo a single phase transition from n = m to m-1 before disappearing above TN(N). This behavior has recently been confirmed by neutron-scattering measurements on CrMn/Cr multilayers. While model I very successfully predicts the behavior of Fe/Cr/Fe wedges, a refined version of model II describes some properties of sputtered Fe/Cr multilayers. [S0163-1829(99)03021-0].
引用
收藏
页码:13849 / 13860
页数:12
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