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

Citation
Rs. Fishman et Zp. Shi, Collinear spin-density-wave ordering in Fe Cr multilayers and wedges, PHYS REV B, 59(21), 1999, pp. 13849-13860
Citations number
44
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B-CONDENSED MATTER
ISSN journal
01631829 → ACNP
Volume
59
Issue
21
Year of publication
1999
Pages
13849 - 13860
Database
ISI
SICI code
0163-1829(19990601)59:21<13849:CSOIFC>2.0.ZU;2-1
Abstract
Several recent experiments have detected a spin-density wave (SDW) within t he Cr spacer of Fe/Cr multilayers and wedges. We use two simple models to p redict the behavior of a collinear SDW within an Fe/Cr/Fe trilayer. Both mo dels combine assumed boundary conditions at the Fe-Cr interfaces with the f ree 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 pe rfect and that the Fe-Cr interaction is antiferromagnetic. Consequently, th e I SDW antinodes lie near the Fe-Cr interfaces. With increasing temperatur e, the Cr spacer undergoes a series of transitions between I SDW phases wit h 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 th e C phase with n = 0 above T-IC(N). For a fixed temperature, the magnetic c oupling across the Cr spacer undergoes a phase slip whenever n changes by o ne. In the limit N--> infinity, T-IC(N) is independent of the Fe-Cr couplin g 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. The se results explain the very high IC transition temperature of about 600 K e xtrapolated 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 e nforced by the interfacial roughness of sputtered Fe/Cr multilayers. As a r esult, the C phase is never stable and the transition temperature T-N(N) ta kes on a seesaw pattern as n greater than or equal to 2 increases with thic kness. In agreement with measurements on both sputtered and epitaxially gro wn 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 sing le 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 propertie s of sputtered Fe/Cr multilayers. [S0163-1829(99)03021-0].