2017
DOI: 10.1103/physrevb.95.224437
|View full text |Cite
|
Sign up to set email alerts
|

Field tuning of domain-wall type and chirality in SrRuO3

Abstract: SrRuO3 films have large uniaxial magnetocrystalline anisotropy tilted out of the film plane. When cooled in zero field from above the Curie temperature (∼ 150 K), a magnetic domain structure emerges in the form of 200 nm wide stripes oriented along the in-plane projection of the magnetic easy axis. We measure the interface resistance of the magnetic domain walls by applying a magnetic field perpendicular to the easy axis in the domain wall plane and perpendicular to this plane and observe hysteretic behavior. … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
3
0

Year Published

2019
2019
2022
2022

Publication Types

Select...
3

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(3 citation statements)
references
References 18 publications
(7 reference statements)
0
3
0
Order By: Relevance
“…First, the medium materials in SRO heterostructures range from complex oxides [34][35][36][37][38][39][40] to metals [41], semiconductors [42] and even two-dimensional (2D) materials [43]. Also, the rich physical properties including high metallic conductivity [23,24], tunable magnetic anisotropy [12,40,44], AHE [22,25,26], magnetic domain walls [45,46], Dzyaloshinskii-Moriya interaction (DMI) [28][29][30], strong SOC strength [22,25,26], variable T C [47] and Weyl fermions [15,27], etc, have also been gradually excavated in SRO-based heterostructures. Finally, in order to effectively control physical properties in heterostructures, various controlling ways have been utilized to modulate the physical properties, including magnetic field [48,49], strain field [50][51][52], electric-field [29,30,[53][54][55], electric-current [12,56], optical [52,57,58]…”
Section: Introductionmentioning
confidence: 99%
“…First, the medium materials in SRO heterostructures range from complex oxides [34][35][36][37][38][39][40] to metals [41], semiconductors [42] and even two-dimensional (2D) materials [43]. Also, the rich physical properties including high metallic conductivity [23,24], tunable magnetic anisotropy [12,40,44], AHE [22,25,26], magnetic domain walls [45,46], Dzyaloshinskii-Moriya interaction (DMI) [28][29][30], strong SOC strength [22,25,26], variable T C [47] and Weyl fermions [15,27], etc, have also been gradually excavated in SRO-based heterostructures. Finally, in order to effectively control physical properties in heterostructures, various controlling ways have been utilized to modulate the physical properties, including magnetic field [48,49], strain field [50][51][52], electric-field [29,30,[53][54][55], electric-current [12,56], optical [52,57,58]…”
Section: Introductionmentioning
confidence: 99%
“…by angle resolved photo‐electron spectroscopy (ARPES). [ 1–9 ] The perovskites SrIrO 3 and SrRuO 3 were shown to exhibit a strong spin Hall effect [ 10,11 ] and to be effective materials for the shifting of magnetic domain walls by electrical currents, [ 12–14 ] respectively. Furthermore, the delafossites PdCoO 2 and PtCoO 2 turned out to be among the most conductive oxides.…”
Section: Introductionmentioning
confidence: 99%
“…
currents, [12][13][14] respectively. Furthermore, the delafossites PdCoO 2 and PtCoO 2 turned out to be among the most conductive oxides.
…”
mentioning
confidence: 98%