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Variation of multilayer magnetoresistance with ferromagnetic layer sequence: Spin-memory loss effects
We find the magnetoresistance (MR) with current flow perpendicular to the layer planes (CPP-MR) of multilayers made of the ferromagnetic metals Co and Py (permalloy = Ni84Fe16) and the nonmagnetic met...

Perpendicular giant magnetoresistance in Co/Cu and permalloy/Cu multilayered nanowires (abstract)

J. Appl. Phys. 81, 4569 (1997); doi:10.1063/1.365430

Issue Date: 15 April 1997

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S. Dubois
UPCPM, place croix du Sud 1, 1348 Louvain la Neuve, Belgium

J. L. Duvail, A. Fert, J. M. George, and J. L. Maurice
Unité Mixte de Physique, CNRS/Thomson, 91404 Orsay, France

L. Piraux
UPCPM, Place croix du Sud 1, 1348 Louvain la Neuve, Belgium
We have prepared Co/Cu and NiFe/Cu (Ni/Fe=permalloy) multilayered nanowires by electrodeposition into pores of membranes or holes made by e-beam lithography in PMMA layers. In both cases, pores and lithography, the diameter of the wires is around 100 nm and the layer thickness ranges between a few nm and several hundred nm. Transmission electron microscopy reveals that the nanowires are composed of long single-crystal grains with c axis (hcp Co) or (111) axis (fcc NiFe or Cu) perpendicular to the axis of the wire. A first series of samples is composed of conventional periodic multilayers. Their CPP-MR ratio can be as large as 80% at 4.2 K (NiFe 5 nm/Cu 5 nm) and giant magnetoresistance effects can be observed up to very large thicknesses (example: tco=1 µm). At small thicknesses, we find the conventional behavior of the so-called "long spin diffusion length limit." More interesting are the results obtained out of this limit and used to determine the spin diffsion length SDL in Cu (140 nm at low T) and Co (44 nm at low T). For NiFe/Cu, the magnetic arrangement of successive layers is more difficult to control and we could not determine the SDL from data of the first series. A second series of samples is made with NiFe/Cu/NiFe trilayers (tCu=10 nm, 7 nm <= tNiFe <= 30 nm), separated from each other by Cu layers of 100 nm. As shown by superconducting quantum interference device measurements, the magnetization of the two NiFe layers in a trilayer are approximately antiparallel at zero field. We use the CPP-MR data on these samples to derive the SDL in permalloy. ©1997 American Institute of Physics.
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KEYWORDS and PACS

Keywords
PACS
  • 75.70.Pa
    Magnetic properties and materials Magnetic films and multilayers Giant magnetoresistance
  • 73.61.At
    Electronic structure and electrical properties of surfaces, interfaces and thin films Electrical properties of specific thin films and layer structures (multilayers, superlattices, quantum wells, wires, and dots) Metal and metallic alloys
  • 73.50.Jt
    Electronic structure and electrical properties of surfaces, interfaces and thin films Electronic transport phenomena in thin films Galvanomagnetic and other magnetotransport effects (including thermomagnetic effects)
  • 75.70.Cn
    Magnetic properties and materials Magnetic films and multilayers Interfacial magnetic properties (multilayers, magnetic quantum wells, superlattices, magnetic heterostructures)
  • 75.50.Bb
    Magnetic properties and materials Studies of specific magnetic materials Fe and its alloys
  • 75.50.Cc
    Magnetic properties and materials Studies of specific magnetic materials Other ferromagnetic metals and alloys
  • 61.46.+w
    Structure of solids and liquids; crystallography Clusters, nanoparticles, and nanocrystalline materials
  • 81.15.Pq
    Materials science Methods of deposition of films and coatings; film growth and epitaxy Electrodeposition, electroplating
  • 68.55.Jk
    Surfaces and interfaces; thin films and whiskers (Structure and nonelectronic properties) Thin film structure and morphology Structure and morphology; thickness
  • YEAR: 1996-97

PUBLICATION DATA

ISSN:
0021-8979 (print)   1089-7550 (online)
Publisher:
AIP is a member of CrossRef AIP

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