2022
DOI: 10.1002/adfm.202206923
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Magnetic Skyrmion Lattices in a Novel 2D‐Twisted Bilayer Magnet

Abstract: Magnetic skyrmions are topologically protected spin swirling vertices, which are promising in device applications due to their particle-like nature and excellent controlability. Magnetic skyrmions are extensively studied in a variety of materials and proposed to exist in the extreme 2D limit, i.e., in twisted bilayer CrI 3 (TBCI). Unfortunately, the magnetic states of TBCIs with small twist angles are disorderly distributed ferromagnetic and antiferromagnetic (AFM) domains in recent experiments, and thus the m… Show more

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Cited by 21 publications
(26 citation statements)
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References 53 publications
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“…Due to so-called stacking-dependent interlayer magnetism, , J ij ⊥ switch from FM to AFM coupling depending on the local stacking pattern between the two magnetic layers (see Supporting Information (SI)). Consequently, the interlayer exchange coupling exhibits the coexistence of AFM and FM interactions in the moiré superlattice accommodating various local stacking patterns (Figure a). , We illustrate this behavior in Figure b through the map of the local interlayer exchange energy J i ⊥ = ∑ j J ij ⊥ computed in an FM configuration S i l = Sẑ . ,,, Specifically, in the monoclinic stacking region (red patches), J i ⊥ exhibits AFM character ( J i ⊥ > 0), indicating a tendency for the spins in the top and bottom layers to align antiparallel to each other. Conversely, in the other stacking regions, J i ⊥ exhibits FM character ( J i ⊥ < 0), signifying a preference for parallel alignment.…”
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confidence: 91%
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“…Due to so-called stacking-dependent interlayer magnetism, , J ij ⊥ switch from FM to AFM coupling depending on the local stacking pattern between the two magnetic layers (see Supporting Information (SI)). Consequently, the interlayer exchange coupling exhibits the coexistence of AFM and FM interactions in the moiré superlattice accommodating various local stacking patterns (Figure a). , We illustrate this behavior in Figure b through the map of the local interlayer exchange energy J i ⊥ = ∑ j J ij ⊥ computed in an FM configuration S i l = Sẑ . ,,, Specifically, in the monoclinic stacking region (red patches), J i ⊥ exhibits AFM character ( J i ⊥ > 0), indicating a tendency for the spins in the top and bottom layers to align antiparallel to each other. Conversely, in the other stacking regions, J i ⊥ exhibits FM character ( J i ⊥ < 0), signifying a preference for parallel alignment.…”
mentioning
confidence: 91%
“…Consequently, the interlayer exchange coupling exhibits the coexistence of AFM and FM interactions in the moirésuperlattice accommodating various local stacking patterns (Figure 2a). [20][21][22][23][24][25]34 We illustrate this behavior in Figure 2b through the map of the local interlayer exchange energy J i ⊥ = ∑ j J ij ⊥ computed in an FM configuration S i l = Sz. 20,22,24,34 Specifically, in the monoclinic stacking region (red patches), J i ⊥ exhibits AFM character (J i ⊥ > 0), indicating a tendency for the spins in the top and bottom layers to align antiparallel to each other.…”
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confidence: 99%
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“…Among various magnetic configurations, magnetic textures with topology protection, such as skyrmions, have garnered significant attention. Skyrmions, characterized by their strong topologically protected stability and small size, are considered the most promising candidates for next-generation information memory devices. The moiré superlattice provides an excellent material system for investigating magnetic textures, as the twisting introduces periodic magnetization domains with complex spin texture. This results in a diverse range of physical images with noncollinear spin configurations, attributed to the modulation of interlayer exchange interaction. ,, Compared to magnetic skyrmions in bulk alloy materials, the magnetic skyrmions in vdW bilayer are significantly thinner, reaching the 2D thickness limit and paving the way for advancements in spin twistronics. …”
Section: Introductionmentioning
confidence: 99%