Bulletin of the American Physical Society
APS March Meeting 2018
Volume 63, Number 1
Monday–Friday, March 5–9, 2018; Los Angeles, California
Session E22: Chiral Magnetism in Thin Films
8:00 AM–11:00 AM,
Tuesday, March 6, 2018
LACC
Room: 402A
Sponsoring
Units:
GMAG DMP
Chair: Adam Ahmed, Ohio State Univ - Columbus
Abstract ID: BAPS.2018.MAR.E22.4
Abstract: E22.00004 : First-principles investigation of chiral magnetic structures in multilayers: {Rh|Co|Pt} and {Pd|Co|Pt}*
8:36 AM–8:48 AM
Presenter:
Stefan Bluegel
(Peter Grünberg Institut and Institute for Advanced Simulation, Forschungszentrum Jülich and JARA)
Authors:
Hongying Jia
(Peter Grünberg Institut and Institute for Advanced Simulation, Forschungszentrum Jülich and JARA)
Bernd Zimmermann
(Peter Grünberg Institut and Institute for Advanced Simulation, Forschungszentrum Jülich and JARA)
Stefan Bluegel
(Peter Grünberg Institut and Institute for Advanced Simulation, Forschungszentrum Jülich and JARA)
Here, we determine the symmetric and antisymmetric magnetic interaction parameters of the magnetic multilayers {Rh|Co|Pt} and {Pd|Co|Pt} using first-principles calculations based on the relativistic full-potential linearized augmented plane-wave (FLAPW) method, as implemented in the FLEUR code (www.flapw.de). We find that the 4d (i.e. Rh and Pd) elements induce a DMI that partly cancels the large DMI produced by the heavy-metal Pt layer. Upon variation of the thickness of the Pt layer between one and five atomic layers, we investigate the interlayer exchange coupling between the magnetic Co layers. For the {Pd|Co|Pt} system, a RKKY-type oscillatory behavior between ferromagnetic and antiferromagnetic interactions is observed. The {Rh|Co|Pt} system has a qualitatively different behavior, where frustrations in between the Co layers lead to a non-collinear order along the c axis.
*Financial support by EU Horizon 2020 via FET-Open project MAGicSky and a JARA-HPC Supercomputing grant.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.MAR.E22.4
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