2022
DOI: 10.1038/s41524-022-00785-9
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Electric-field driven stability control of skyrmions in an ultrathin transition-metal film

Abstract: To realize future spintronic applications with magnetic skyrmions—topologically nontrivial swirling spin structures—it is essential to achieve efficient writing and deleting capabilities of these quasi-particles. Electric-field assisted nucleation and annihilation is a promising route, however, the understanding of the underlying microscopic mechanisms is still limited. Here, we show how the stability of individual magnetic skyrmions in an ultrathin transition-metal film can be controlled via external electric… Show more

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Cited by 10 publications
(12 citation statements)
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“…The variation of the different magnetic interactions due to the applied electric field can be explained based on the spin-dependent screening charge in the film as discussed in detail in Refs. [36,40]. Note, that electric-field effects on the exchange interaction which are even by a factor of about two larger than in Pd/Fe/Ir(111) have been reported based on DFT studies for film systems with a Co [36] or an Fe [40] monolayer directly at the surface.…”
Section: F Electric-field Assisted Switchingmentioning
confidence: 89%
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“…The variation of the different magnetic interactions due to the applied electric field can be explained based on the spin-dependent screening charge in the film as discussed in detail in Refs. [36,40]. Note, that electric-field effects on the exchange interaction which are even by a factor of about two larger than in Pd/Fe/Ir(111) have been reported based on DFT studies for film systems with a Co [36] or an Fe [40] monolayer directly at the surface.…”
Section: F Electric-field Assisted Switchingmentioning
confidence: 89%
“…[36,40]. Note, that electric-field effects on the exchange interaction which are even by a factor of about two larger than in Pd/Fe/Ir(111) have been reported based on DFT studies for film systems with a Co [36] or an Fe [40] monolayer directly at the surface. The induced change in the exchange constant J 1 amounts to ∆J 1 = ±0.29 meV for an electric field of E = ±0.5 V/ Å (cf.…”
Section: F Electric-field Assisted Switchingmentioning
confidence: 89%
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