2022
DOI: 10.1016/j.actamat.2022.118383
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Compositional gradient induced enhancement of Dzyaloshinskii–Moriya interaction in Pt/Co/Ta heterostructures modulated by Pt–Co alloy intralayers

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Cited by 9 publications
(4 citation statements)
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“…Most of the papers investigating micromagnetic features in Co-Pd based films consider multilayer structures with sharp interfaces and pre-set Co versus Pd composition (either pure Co/Pd multilayer or CoPd solid solutions with digital content variation). [21][22][23][24]58] Smaller number of papers is considered slightly mixed layers with an intermediate 4-6 monolayer thick area. [26,59,60] Unlike the majority of the papers, the structures in the present study are highly intermixed Co x Pd 1-x films with unfixed Co versus Pd content.…”
Section: Resultsmentioning
confidence: 99%
“…Most of the papers investigating micromagnetic features in Co-Pd based films consider multilayer structures with sharp interfaces and pre-set Co versus Pd composition (either pure Co/Pd multilayer or CoPd solid solutions with digital content variation). [21][22][23][24]58] Smaller number of papers is considered slightly mixed layers with an intermediate 4-6 monolayer thick area. [26,59,60] Unlike the majority of the papers, the structures in the present study are highly intermixed Co x Pd 1-x films with unfixed Co versus Pd content.…”
Section: Resultsmentioning
confidence: 99%
“…The effective field in CoTbPt has been proposed to have originated from the inversion symmetry-breaking by introducing the vertical gradient compositions of Pt, which, in combination with SOT, can lead to the deterministic field-free SOT switching in the absence of an external field. When there is a composition gradient of Pt in the ferrimagnetic layer, it can induce a gradient-driven bulk Dzyaloshinskii–Moriya interaction (b-DMI). While the b-DMI is defined by the presence of composition differences and structure symmetry which can break the chiral symmetry and determine the SOT switching without an external field. , The absence of SOT switching at H x = −13 Oe indicates the effective field of −13 Oe, which is canceled by the external field and results in the nondeterministic SOT switching. It is worth noticing that the switching ratio of R Hall is gradually reduced at a larger H x , i.e., a multi-state behavior.…”
Section: Resultsmentioning
confidence: 99%
“…The present experiment also indicates that the magnitude of the effective structure symmetry which can break the chiral symmetry and determine the SOT switching without an external field. 52,53 The absence of SOT switching at H x = −13 Oe indicates the effective field of −13 Oe, which is canceled by the external field and results in the nondeterministic SOT switching. It is worth noticing that the switching ratio of R Hall is gradually reduced at a larger H x , i.e., a multi-state behavior.…”
Section: ■ Introductionmentioning
confidence: 99%
“…Recently, the Dzyaloshinskii–Moriya interaction (DMI) has gained much attention since it is recognized to play an essential role in a broad range of physical phenomena, such as the observation of magnetic skyrmions, fast current-controlled domain wall motion, , magnetoelectric effect, , topological Hall effect, and magnetization switching. , The emergence of DMI requires the breaking of inversion symmetry in the spin system with spin–orbit coupling (SOC). , In magnetic multilayers, it is usually believed that the disorders like the intermixing and dusting of elements at interfaces are detrimental to the interfacial DMI. , Interestingly, recent experiments have observed a significant DMI (termed g-DMI hereafter) in the amorphous thin films with a composition gradient to break the inversion symmetry. The measured DMI value shows a linear relation with the film thickness, signifying a bulk nature of g-DMI despite in the thin films.…”
mentioning
confidence: 99%