2021
DOI: 10.1016/j.physrep.2020.10.001
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Beyond skyrmions: Review and perspectives of alternative magnetic quasiparticles

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Cited by 440 publications
(322 citation statements)
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“…An enormous effort has been undertaken to find solutions for suppressing this so called skyrmion Hall effect, for example modifying the spin torque 27,28 or using alternative magnetic quasiparticles 29 with a vanishing topological charge (like antiferromagnetic skyrmions [30][31][32][33][34][35] or skyrmioniums [36][37][38] or nano-objects with a broken rotational symmetry (like antiskyrmions 39,40 or bimerons 28,41,42 ). However, as we show in the present paper, the skyrmion Hall effect may even be a favorable feature that can be utilized instead of trying to suppress it.…”
mentioning
confidence: 99%
“…An enormous effort has been undertaken to find solutions for suppressing this so called skyrmion Hall effect, for example modifying the spin torque 27,28 or using alternative magnetic quasiparticles 29 with a vanishing topological charge (like antiferromagnetic skyrmions [30][31][32][33][34][35] or skyrmioniums [36][37][38] or nano-objects with a broken rotational symmetry (like antiskyrmions 39,40 or bimerons 28,41,42 ). However, as we show in the present paper, the skyrmion Hall effect may even be a favorable feature that can be utilized instead of trying to suppress it.…”
mentioning
confidence: 99%
“…We begin by recalling that in non relativistic 3D quantum mechanics, the spin states S z , S ji of spinfull particles are characterised by two half integers S z , S ðÞ ,a positive S ≥ 0 and an S z taking 2S þ 1 values bounded as ÀS ≤ S z ≤ S with integral hoppings. For particles with spin 1/2 like electrons, one distinguishes two basis vector states AE 1 2 , 1 2 that are eigenvalues of the scaled Pauli matrix ℏ 2 σ z and the quadratic (Casimir) operator . From these ingredients, we learn that the average…”
Section: Quantum Spin 1/2 Operator and Beyondmentioning
confidence: 99%
“…For generic values of the SU 2 ðÞspin S, the spin operator reads as ℏJ a where the three J a 's are 2S þ 1 ðÞ Â 2S þ 1 ðÞ generators of the SU 2 ðÞgroup satisfying the usual commutation relations J a , J b ½ ¼ iε abc J c with ε abc standing for the completely antisymmetric Levi-Civita tensor with non zero value ε 123 ¼ 1; its inverse is ε cba with ε 123 ¼À1. The time evolution of the spin 1 2 operator ℏ σ a 2 with dynamics governed by a stationary Hamiltonian operator (dH=dt ¼ 0) is given by the Heisenberg representation of quantum mechanics. In this non dissipative description, the time dependence of the spin 1 2 operatorŜ a t ðÞ (the hat is to distinguish the operatorŜ a from classical S a ) is given bŷ…”
Section: Quantum Spin 1/2 Operator and Beyondmentioning
confidence: 99%
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“…In magnetism, non-collinear spin textures can also be characterized by a topological invariant, albeit defined in real space. This 'topological charge' or 'skyrmion number' Nsk is ±1 for most of the recently observed objects 11,12 , including skyrmions and antiskyrmions, which are mesoscopic magnetic whirls that have been observed in chiral systems [13][14][15] . An integer value of Nsk is guaranteed under the assumption of a continuous spin texture and that the surface on which it resides (the magnetic unit cell or the whole sample depending on the periodicity of the texture) can be mapped to a sphere.…”
Section: Introductionmentioning
confidence: 99%