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Skyrmion lattice defects
a Visualisation of an edge dislocation in a skyrmion crystal. This dislocation manifests itself as a topological defect, which can be thought of as one skyrmion gaining a nearest neighbour from an adjacent skyrmion; the Voronoi cells surrounding the skyrmions with 5 and 7 nearest neighbours are coloured yellow and green, respectively. This so-called 5–7 defect can glide along its Burgers vector, indicated by b, costing very little energy. The Burgers vector of a 5–7 defect must lie along a real lattice basis vector²⁸. Were the lattice sheared vertically, strain could be efficiently relieved by propagation of the pictured 5–7 defect along its Burgers vector. b Idealized visualization of the diffraction pattern from a strained 2D crystal with a 5–7 defect. Strain in the vicinity of the defect elongates four of the peaks anisotropically: the Burgers vector specifies a unique direction and its corresponding defect breaks the six-fold symmetry of the hexagonal lattice³⁴.

Skyrmion lattice defects a Visualisation of an edge dislocation in a skyrmion crystal. This dislocation manifests itself as a topological defect, which can be thought of as one skyrmion gaining a nearest neighbour from an adjacent skyrmion; the Voronoi cells surrounding the skyrmions with 5 and 7 nearest neighbours are coloured yellow and green, respectively. This so-called 5–7 defect can glide along its Burgers vector, indicated by b, costing very little energy. The Burgers vector of a 5–7 defect must lie along a real lattice basis vector²⁸. Were the lattice sheared vertically, strain could be efficiently relieved by propagation of the pictured 5–7 defect along its Burgers vector. b Idealized visualization of the diffraction pattern from a strained 2D crystal with a 5–7 defect. Strain in the vicinity of the defect elongates four of the peaks anisotropically: the Burgers vector specifies a unique direction and its corresponding defect breaks the six-fold symmetry of the hexagonal lattice³⁴.

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... The magnitude of this Hall angle increases linearly with , escalating by a factor of 40 as progresses from 0.1 to 1, while the skyrmion's velocity experiences only a slight rise from 280 to 300 m/s (see Fig. 7(b)). Our investigation affirms the theoretical projections [25,[72][73][74], that skyrmions of opposing polarities present Hall angles that are equal in magnitude yet opposite in sign. Thus replacing a skyrmion with opposite polarity but the same chirality results in Hall angles at different values that are equal in size but opposite in direction. ...
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... In this geometry, the coexistence between various states is easily observed, since the states are remarkably similar in free energy [23]. This coexistence is easily achieved in real samples and has the potential to be utilised within skyrmionic devices, as these states occupy local minima within the magnetic Hamiltonian, and as such have repulsive interactions [27]. ...
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