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024 7 _ |a 10.1103/PhysRevB.79.094411
|2 DOI
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041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |0 P:(DE-HGF)0
|a Hardrat, B.
|b 0
245 _ _ |a Complex Magnetism of Iron Monolayers on Hexagonal Transition Metal Surfaces from First Principles
260 _ _ |a College Park, Md.
|b APS
|c 2009
300 _ _ |a 094411- 094416
336 7 _ |a Journal Article
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440 _ 0 |0 4919
|a Physical Review B
|v 79
|x 1098-0121
|y 9
500 _ _ |a Financial support of the Stifterverband fur die Deutsche Wissenschaft, the Interdisciplinary Nanoscience Center Hamburg, and the ESF EUROCORES Programme SONS under Contract No. ERAS-CT-2003-980409 is gratefully acknowledged.
520 _ _ |a Using first-principles calculations, we demonstrate that an Fe monolayer can assume very different magnetic phases on hcp (0001) and fcc (111) surfaces of 4d- and 5d-transition metals. Due to the substrates' d-band filling, the nearest-neighbor exchange coupling of Fe changes gradually from antiferromagnetic (AFM) for Fe films on Tc, Re, Ru, and Os to ferromagnetic on Rh, Ir, Pd, and Pt. In combination with the topological frustration on the triangular lattice of these surfaces the AFM coupling results in a 120 degrees Neel structure for Fe on Re and Ru and an unexpected double-row-wise AFM structure on Rh, which is a superposition of left- and right-rotating 90 degrees spin spirals.
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653 2 0 |2 Author
|a antiferromagnetic materials
653 2 0 |2 Author
|a exchange interactions (electron)
653 2 0 |2 Author
|a ferromagnetic-antiferromagnetic transitions
653 2 0 |2 Author
|a iron
653 2 0 |2 Author
|a magnetic thin films
653 2 0 |2 Author
|a monolayers
653 2 0 |2 Author
|a Neel temperature
653 2 0 |2 Author
|a surface magnetism
700 1 _ |0 P:(DE-Juel1)130498
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700 1 _ |0 P:(DE-HGF)0
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700 1 _ |0 P:(DE-Juel1)130548
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700 1 _ |0 P:(DE-Juel1)130545
|a Bihlmayer, G.
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700 1 _ |0 P:(DE-HGF)0
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773 1 8 |a 10.1103/physrevb.79.094411
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773 _ _ |a 10.1103/PhysRevB.79.094411
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