Fig. 5: Current-driven motion of various magnetic skyrmionic structures on the racetrack without the skyrmion Hall effect. | Nature Communications

Fig. 5: Current-driven motion of various magnetic skyrmionic structures on the racetrack without the skyrmion Hall effect.

From: Magnetic skyrmionic structures with variable topological charges in engineered Dzyaloshinskii-Moriya interaction systems

Fig. 5

ac Spin-transfer-torque drives the skyrmion (a), antiskyrmion (b), and high-Q skyrmionic structure (c) to move along the DMI-engineered racetrack. The dotted line marks the initial position of the magnetic skyrmionic structures. d Various skyrmionic structures’ velocity v as a function of electrical current density j. The empty symbols mean that the skyrmionic structures will annihilate at the present current density.

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