Contents lists available at ScienceDirect Journal of Magnetism and Magnetic Materials journal homepage: www.elsevier.com/locate/jmmm Research articles Inuence 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-eld Detection, College of Science, China Three Gorges of University, Yichang 443002, China ARTICLE INFO Keywords: Spin Hall magnetoresistance Spin Hall eects Spin current absorption Anisotropic magnetoresistance Spin current transportation ABSTRACT The spin Hall magnetoresistance eects (SMR) in four heterostructures consist of dierent boundaries of Pt layer has been investigated. The result in this work shows that the two boundaries of Pt layer in all heterostructures both inuence the spin current absorption and reection. 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 eect 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 eect (SHE) [13], inverse spin Hall eect (ISHE) [4,5], spin pumping [6,7], spin Seebeck eect (SSE) [8,9], spin-dependent thermoelectric eect [10,11], spin Peltier eect (SPE) [12,13], and spin Hall magnetoresistance (SMR) [1416]. 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 [1719]. Strong spin-orbit coupling exists in the interface between the HM layer and the FM one. Many factors aect the spin current absorption and reection 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 eect which is the collective eect 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 [2426] on the SMR in YIG/antiferromagnetic insulator (AFI)/Pt and AFI/Pt heterostructures indicates that spin mixing conductance could be enhanced signicantly when the thickness of the AFI increases from zero to several nanometers. Spin ip 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 inuence the SMR signicantly. The spin current can be generated in the HM layer connected with FM due to SOC. However, many factors aect the spin current absorption and reection at the FM/HM interface. The HM layer with spin current transporting in it has two boundaries around it. In addition, the spin diusion 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 dierent kinds of heterostructures with the Pt layer having dierent boundaries. The work shows that dierent boundaries of the Pt layer inuence the spin current absorption signicantly. 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. T