TY - JOUR
T1 - Giant monolayer magnetization of Fe on MgO
T2 - A nearly ideal two-dimensional magnetic system
AU - Li, Chun
AU - Freeman, Arthur J
PY - 1991/1/1
Y1 - 1991/1/1
N2 - Studies of the structural, electronic, and magnetic properties of a model 3d ferromagnetic metal-ceramic interface system Fe/MgO(001) by the full-potential linearized augmented-plane-wave total-energy method are reported. Surprisingly, the electronic and magnetic properties of a monolayer of Fe on MgO(001) substrate (magnetic moment M=3.07B) are remarkably close to that of a free-standing Fe monolayer (with a giant moment M=3.10B), as a result of the lack of electronic interaction between Fe and MgO. (The charge transfer at the Fe/MgO interface is less than 0.05 e/atom and so any direct chemical interaction between Fe and MgO is unlikely.) Thus, this system might be an ideal two-dimensional system for studying other phenomena such as magnetic anisotropy, phase transitions, and critical behavior. For two layers of Fe on MgO, i.e., 2Fe/MgO(001), the top layer Fe(M=2.96B) shows features close to that of a free bcc Fe(001) surface (M=2.96B). Significantly, the magnetic moment of the Fe layer that interfaces the MgO substrate (M=2.85B) is also largely enhanced from the subsurface moment (2.35B) in bcc Fe(001), again indicating an extremely weak effect from the MgO substrate.
AB - Studies of the structural, electronic, and magnetic properties of a model 3d ferromagnetic metal-ceramic interface system Fe/MgO(001) by the full-potential linearized augmented-plane-wave total-energy method are reported. Surprisingly, the electronic and magnetic properties of a monolayer of Fe on MgO(001) substrate (magnetic moment M=3.07B) are remarkably close to that of a free-standing Fe monolayer (with a giant moment M=3.10B), as a result of the lack of electronic interaction between Fe and MgO. (The charge transfer at the Fe/MgO interface is less than 0.05 e/atom and so any direct chemical interaction between Fe and MgO is unlikely.) Thus, this system might be an ideal two-dimensional system for studying other phenomena such as magnetic anisotropy, phase transitions, and critical behavior. For two layers of Fe on MgO, i.e., 2Fe/MgO(001), the top layer Fe(M=2.96B) shows features close to that of a free bcc Fe(001) surface (M=2.96B). Significantly, the magnetic moment of the Fe layer that interfaces the MgO substrate (M=2.85B) is also largely enhanced from the subsurface moment (2.35B) in bcc Fe(001), again indicating an extremely weak effect from the MgO substrate.
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U2 - 10.1103/PhysRevB.43.780
DO - 10.1103/PhysRevB.43.780
M3 - Article
AN - SCOPUS:25544431516
SN - 0163-1829
VL - 43
SP - 780
EP - 787
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 1
ER -