Issue |
Europhys. Lett.
Volume 49, Number 4, February II 2000
|
|
---|---|---|
Page(s) | 528 - 533 | |
Section | Condensed matter: electronic structure, electrical, magnetic, and optical properties | |
DOI | https://doi.org/10.1209/epl/i2000-00182-9 | |
Published online | 01 September 2002 |
Inverse giant magnetoresistance in rare-earth/transition metal multilayers
1
E. C. Stoner Laboratory, Department of Physics
and Astronomy University of Leeds -
Leeds, LS2 9JT, UK
2
ISIS, Rutherford Appleton Laboratory - Chilton,
Didcot, Oxon, OX11 0QX, UK
Received:
19
August
1999
Accepted:
3
December
1999
Giant magnetoresistance (GMR) is observed in multilayered
structures with 3d ferromagnetic layers separated by normal metal
spacer layers, and is usually a negative magnetoresistance. No GMR
has been observed to date in multilayers with solely 4f
ferromagnetic layers. Nevertheless, in a hybrid 3d/4f magnetic
multilayer of the form an inverse
GMR of up to
has been measured at 4.2 K. This effect is
explained in terms of a spin-engineered configuration of layers
which forces the moments of adjacent Co layers to be anti-parallel
in a high-field state, and parallel in a low-field state. Since
the structure is formed from separate magnetic layers, it has been
shown, by varying the order of the layers, that Co/Cu interfaces
are essential to the GMR in these types of structures. Although
there is no GMR in rare-earth/non-magnetic multilayers, the Dy
layers are sufficiently transparent to electrons for the GMR to
continue rising as the number of repeat units is increased, up to
N = 4.
PACS: 75.70.Pa – Giant magnetoresistance / 71.20.Eh – Rare earth metals and alloys / 71.20.Be – Transition metals and alloys
© EDP Sciences, 2000
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