2020
DOI: 10.1103/physrevb.101.134420
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Skyrmions and spin waves in frustrated ferromagnets at low applied magnetic field

Abstract: A continuum model of frustrated ferromagnets is analyzed in detail in the regime of low applied magnetic field, H 0 < 1/4, where the ground state is a spatially varying conical spiral. By changing variables to a corotating spin field, the model is reformulated as a gauged sigma model in a fixed background gauge, allowing the construction of stable isolated Skyrmions, and stable multi-Skyrmion clusters, which approach the conical ground state at spatial infinity. Owing to the spatial anisotropy induced by the g… Show more

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Cited by 10 publications
(4 citation statements)
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“…Example solutions of solvable rank one models and their properties are discussed in [10] and also [16]. We note that a similar reformulation in terms of a flat gauge field was recently applied to a rather different ferromagnetic model in [17].…”
Section: Examplesmentioning
confidence: 88%
“…Example solutions of solvable rank one models and their properties are discussed in [10] and also [16]. We note that a similar reformulation in terms of a flat gauge field was recently applied to a rather different ferromagnetic model in [17].…”
Section: Examplesmentioning
confidence: 88%
“…We then evolve the system in eq. 1, using a gradient decent method, in particular an arrested Newton flow algorithm (described in detail in [32]), solving for the motion of a particle in C under the potential F dis , φ = −gradF dis (φ), (A1)…”
Section: Discussionmentioning
confidence: 99%
“…24 according to our chosen orthonormal basis {x 1 , x2 , x3 }. We then solved the resulting 1-dimensional boundary problem (where H purely fixes the boundary conditions), using a Newton flow algorithm [32] which we describe briefly in appendix A.…”
Section: A Meissner State Solutionsmentioning
confidence: 99%
“…The baby Skyrme energy is then discretised using a 4th order central finite-difference scheme. This yields a discrete approximation E dis [ϕ] to the static energy functional E[ϕ], which we can regard as a function E dis : C → R, where the discretised configuration space is the manifold C = (S 2 ) N1 N2 ⊂ R 3 N1 N2 [26,27].…”
Section: A Initial Configurationsmentioning
confidence: 99%