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Journal of Magnetism and Magnetic Materials
journal homepage: www.elsevier.com/locate/jmmm
Research articles
Influence of the two boundaries of the Pt layer on spin current
transportation by spin Hall magnetoresistance
Zhiwen Dai, Xiufeng Huang
⁎
, Dongchao Yang, Lizhi Yi, Fengyu Wu, Hongguang Piao, Liqing Pan
⁎
Research Institute for Magnetoelectronics & Weak Magnetic-field Detection, College of Science, China Three Gorges of University, Yichang 443002, China
ARTICLE INFO
Keywords:
Spin Hall magnetoresistance
Spin Hall effects
Spin current absorption
Anisotropic magnetoresistance
Spin current transportation
ABSTRACT
The spin Hall magnetoresistance effects (SMR) in four heterostructures consist of different boundaries of Pt layer
has been investigated. The result in this work shows that the two boundaries of Pt layer in all heterostructures
both influence the spin current absorption and reflection. The Pt/air interface would weaken the spin current
absorption at the Co
2
FeSi/Pt interface on the other side of the Pt layer. On the contrary, the Pt/MgO(0 0 1)
interface could boost the spin current absorption strongly at the Co
2
FeSi/Pt interface on the other side of the Pt
layer. And this promotion effect is much stronger than the Co
2
FeSi/Pt interface on the spin current absorption at
the other Co
2
FeSi/Pt interface. The MgO capping layer may avoid anisotropic magnetoresistance (AMR) induced
SMR ratio decreasing at low temperature. This study provides a new way for modulating spin current absorption
at the FM/HM interface.
1. Introduction
The generation, transportation and detection of pure spin current
are central issues in spintronics. There are many physical phenomena
are related to pure spin current, such as spin Hall effect (SHE) [1–3],
inverse spin Hall effect (ISHE) [4,5], spin pumping [6,7], spin Seebeck
effect (SSE) [8,9], spin-dependent thermoelectric effect [10,11], spin
Peltier effect (SPE) [12,13], and spin Hall magnetoresistance (SMR)
[14–16]. All these phenomena involve spin current transportation in
heavy metal (HM) layer contacted with ferromagnetic (FM) layer. The
FM layer can be insulator, semiconductor, or metal [17–19]. Strong
spin-orbit coupling exists in the interface between the HM layer and the
FM one. Many factors affect the spin current absorption and reflection
at the FM/HM interface. The spin Hall angle which represents the
strength of the spin-orbit coupling is a dominant one [20]. The property
of the FM/HM interface plays an important role as well [21]. Recent
study shows that spatial distribution of spin current is more compli-
cated in FM/HM based multilayer structure compared to FM/HM single
bilayer structure [22]. Several spin current related phenomena in HM/
FM based multilayer structures such as SSE and SPE indicate that the
magnitude of the spin current in the middle layer is largest. It becomes
smaller and smaller when the spin currents distribute in the layer away
from the middle one [23].
Spin Hall magnetoresistive effect which is the collective effect of
SHE and ISHE attracts great interest of people in recent years.
Therefore, SMR can be used as a practical method for the study of spin
current generation, propagation and detection. The latest research
[24–26] on the SMR in YIG/antiferromagnetic insulator (AFI)/Pt and
AFI/Pt heterostructures indicates that spin mixing conductance could
be enhanced significantly when the thickness of the AFI increases from
zero to several nanometers. Spin flip may occur at the AFI/Pt interface
when the AFI exchanges coupled with YIG at low temperature. These
researches show that magnetic microstructure at the interface influence
the SMR significantly. The spin current can be generated in the HM
layer connected with FM due to SOC. However, many factors affect the
spin current absorption and reflection at the FM/HM interface. The HM
layer with spin current transporting in it has two boundaries around it.
In addition, the spin diffusion length in the HM layer is only several
nanometers. It is not clear that apart from the FM/HM boundary,
whether another boundary of the HM layer participates in the spin
current transportation.
In this paper, we investigate the two boundaries of the Pt layer on
spin current transportation by using spin Hall magnetoresistance. We
report the SMR in different kinds of heterostructures with the Pt layer
having different boundaries. The work shows that different boundaries
of the Pt layer influence the spin current absorption significantly. This
study provides a new way for modulating spin current absorption from
HM layer to the FM layer.
2. Experimental
In this experiment, four heterostructures, from bottom to top, MgO
https://doi.org/10.1016/j.jmmm.2018.06.060
Received 2 May 2018; Received in revised form 12 June 2018; Accepted 19 June 2018
⁎
Corresponding author.
E-mail addresses: xiufenghuang@ctgu.edu.cn (X. Huang), lpan@ctgu.edu.cn (L. Pan).
Journal of Magnetism and Magnetic Materials 465 (2018) 585–589
Available online 20 June 2018
0304-8853/ © 2018 Elsevier B.V. All rights reserved.
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