2018
DOI: 10.1038/s41598-017-18369-9
|View full text |Cite
|
Sign up to set email alerts
|

Interface-induced spin Hall magnetoresistance enhancement in Pt-based tri-layer structure

Abstract: In this study, we integrated bilayer structure of covered Pt on nickel zinc ferrite (NZFO) and CoFe/Pt/NZFO tri-layer structure by pulsed laser deposition system for a spin Hall magnetoresistance (SMR) study. In the bilayer structure, the angular-dependent magnetoresistance (MR) results indicate that Pt/NZFO has a well-defined SMR behavior. Moreover, the spin Hall angle and the spin diffusion length, which were 0.0648 and 1.31 nm, respectively, can be fitted by changing the Pt thickness in the longitudinal SMR… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
3
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 5 publications
(3 citation statements)
references
References 37 publications
0
3
0
Order By: Relevance
“…The most well-known form of MPE is where a thin interfacial region in the nonmagnetic metal exhibits an induced moment through exchange with the magnetic layer. However, there are closely related effects, such as interface-induced spin anisotropy and dynamic MPE, which can also be considered proximity effects, although these do not necessarily lead to a locally modified magnetization magnitude [16]. MPE-induced magnetism contributes to the HM's magnetoresistance and couples to the ferromagnet's magnetic moment, making the MPE an essential element in defining the behavior of HM/magnetic heterostructures, especially at low temperatures where the MPE is stronger.…”
Section: Introductionmentioning
confidence: 99%
“…The most well-known form of MPE is where a thin interfacial region in the nonmagnetic metal exhibits an induced moment through exchange with the magnetic layer. However, there are closely related effects, such as interface-induced spin anisotropy and dynamic MPE, which can also be considered proximity effects, although these do not necessarily lead to a locally modified magnetization magnitude [16]. MPE-induced magnetism contributes to the HM's magnetoresistance and couples to the ferromagnet's magnetic moment, making the MPE an essential element in defining the behavior of HM/magnetic heterostructures, especially at low temperatures where the MPE is stronger.…”
Section: Introductionmentioning
confidence: 99%
“…Since the first pioneering experiment one branch of research deals with investigating the SMR in all-metallic multilayers; however, the outcome is not conclusive. As also pointed out by Zou et al [45] the structural properties, particularly the crystallinity of the films, are mandatory for a profound interpretation of MR data; however, they are often disregarded or not considered [34,[40][41][42][55][56][57][58][59] even in carefully performed studies [60,61]. Frequently, Δρ op signatures are ad hoc interpreted to be a fingerprint of the SMR while not thoroughly proven whether crystalline or interfacial AMR effects exist [34,[39][40][41][42][55][56][57][58][59]62].…”
mentioning
confidence: 99%
“…Frequently, Δρ op signatures are ad hoc interpreted to be a fingerprint of the SMR while not thoroughly proven whether crystalline or interfacial AMR effects exist [34,[39][40][41][42][55][56][57][58][59]62]. The studies particularly lack an appropriate modeling of the electronic transport in all-metallic layered structures including the consideration of interface-scattering processes [39][40][41][42][55][56][57][58][59][60][61]63]. Properly correcting for the current shunt through paramagnetic layers provides the feasibility for the separation of interface and bulklike MR contributions [30], which is a necessary prerequisite to check for the validity of Eq.…”
mentioning
confidence: 99%