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Antiferromagnetic interlayer exchange coupling in Pt/Co multilay...
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磁各向异性垂直于膜面的Co/Pt多层膜中的反铁磁层间交换耦合,柳忠元,张芳,通过采用超薄NiO层取代Pt保护层,我们给出了Co/Pt多层膜中存在反铁磁层间耦合的直接实验证据。NiO层在反铁磁层间耦合的观测中起到两�
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1
Antiferromagnetic interlayer exchange coupling
in Pt/Co multilayers with perpendicular anisotropy
Z.Y. Liu, F. Zhang, H.L. Chen, B. Xu, D.L. Yu, J.L. He, Y.J. Tian
State Key Laboratory of Metastable Materials Science & Technology,
Yanshan University, Qinhuangdao 066004, China
Email:
liuzy0319@yahoo.com, fhcl@ysu.edu.cn
Abstract
By using one ultrathin NiO layer to replace the Pt capping layer in the Co/Pt
multilayer with perpendicular anisotropy, we present direct evidence for the existence
of antiferromagnetic interlayer coupling between the Co layers through the Pt layers
thicker than 24 Å. The NiO capping layers play two key roles in the observation of
antiferromagnetic interlayer coupling. One is the manipulation of the coercivity of the
Co layer in contact with the NiO layer, the other is the enhancement of the electron
reflectivities at the Co/Pt interfaces via the specular scattering effect at the Co-NiO
interface. The thermal variation of the magnetization of the Co layer also plays an
important role in the observed antiferromagnetic coupling due to its strong effect on the
phase of electron reflectivity at the Co/Pt interfaces. The magnetization-dependent
phase can lead to the ferromagnetic-antiferromagnetic transition of the interlayer
coupling at high temperature. All these factors are combined together to realize the
direct observation of antiferromagnetic interlayer coupling in the Co/Pt multilayer with
perpendicular anisotropy.
Keywords: Antiferromagnetic interlayer coupling; Co/Pt multilayer;
Perpendicular anisotropy
http://www.paper.edu.cn
2
1 Introduction
Since the discovery of the antiferromagnetic (AF) interlayer exchange coupling (IEC)[1] and
giant magnetoresistance (GMR)[2] in the layered ferromagnetic (FM) films separated by the
metallic Cr spacers, these phenomena have been subjects of great interest. A variety of
nonmagnetic spacer materials have been investigated and the AF IEC has been observed, for
example, the transition metals[3, 4] To date, most of the layered FM films with the AF IEC have
the in-plane anisotropy. In recent years, the observations of the AF IEC in the layered FM films
with the perpendicular anisotropy[5]-[7] have stimulated intensive investigations on the these
artificial antiferromagnets.[8]-[14] For their design, the Pt/Co multilayers have been often taken as
the FM building blocks. However, the IEC between the Co layers via the Pt layers has been an
intriguing problem in the Pt/Co multilayers themselves. For the transition-metallic Pt spacers,
although the theoretical calculations predict the existence of the AF IEC,[15] the previous
experimental studies have revealed only the FM IEC with the oscillatory coupling strength as a
function of the Pt layer thickness resulting from the RKKY-type interactions.[16, 17] The
polarization of the Pt layers owing to the Co 3d-Pt 5d hybridization at the Pt/Co interfaces, which
makes the Pt layers become weakly FM, are considered to play an important role in the FM
IEC.[17]
Understanding the IEC in the Pt/Co multilayers is significant for the design of the
artificial antiferromagnets with perpendicular anisotropy[14] and their applications in spintronic
devices.[18]
In the present work, our experimental investigations on the [Pt/Co]
3
mutliayers capped by one
ultrathin NiO layer have presented unambiguous evidence for the existence of AF IEC between
the Co layers across the Pt layers with thickness larger than 24 Å. This AF IEC is found to be
thermally dependent, and is very sensitive to the thicknesses of the NiO capping layer and the Pt
layer.
2 Sample preparation and measurements
The samples with the configuration of [Pt(t
Pt
Å)/Co(4 Å)]
3
/NiO(t
NiO
Å) were prepared onto the
glass substrates covered with 100 Å Pt buffer layer using the dc and rf magnetron sputtering in 4
mTorr Ar pressure. The base pressure before deposition was 4x10
-7
Torr. The deposition rates from
the Pt (99.95%), Co (99.9%), and NiO (98%) targets were calibrated to be 0.28. 0.18, and 0.21 Å
/s, respectively. X-ray diffraction measurements display that the samples are highly fcc(111)
textured, and the grazing incident X-ray reflectivity confirms the high quality of the interfaces.
The measurements of extraordinary Hall effect (EHE) and magnetoresistance (MR) were
performed in PPMS (QuantumDesign) with the magnetic field and the current applied
out-of-plane and in-plane, respectively.
http://www.paper.edu.cn
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