2000
DOI: 10.1134/1.568329
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Dispersion relation for kink-type solitons in one-dimensional ferromagnets

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Cited by 15 publications
(11 citation statements)
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“…It is important, however, that the difference of the momenta for two different states of the DW is a gauge-invariant quantity. 29 To show this, let us imagine the DW as a trajectory in spin space { S}, S = S(ξ). The trajectories emerging from one point, say, S = S( e x sin θ 0 − e z cos θ 0 ) and ending at another point S = S( e x sin θ 0 + e z cos θ 0 ) can be associated with DW's that move with different velocities but obey identical boundary conditions at infinity.…”
Section: Domain Wall Dynamics In Continuum Approximationmentioning
confidence: 99%
See 1 more Smart Citation
“…It is important, however, that the difference of the momenta for two different states of the DW is a gauge-invariant quantity. 29 To show this, let us imagine the DW as a trajectory in spin space { S}, S = S(ξ). The trajectories emerging from one point, say, S = S( e x sin θ 0 − e z cos θ 0 ) and ending at another point S = S( e x sin θ 0 + e z cos θ 0 ) can be associated with DW's that move with different velocities but obey identical boundary conditions at infinity.…”
Section: Domain Wall Dynamics In Continuum Approximationmentioning
confidence: 99%
“…For the near Heisenberg antiferromagnets with weak anisotropy of any origin, exchange or single-ion, treated on the basis of the sigma-model, the singularities in the Lagrangian for the staggered magnetization are absent for a sufficiently general set of models (including antiferromagnets subject to strong external magnetic fields and in the presence of Dzyaloshinski-Moriya interactions of arbitrary symmetry 36 ) and a periodic DW dispersion law is not realized. 29 Another interesting feature, which is common to classical and quantum physics, is that states with finite range of motion for the coordinate, but infinite range for momentum are present for large enough pinning potential, U 0 > T 0 . Evidently such trajectories do not exist for standard mechanical systems with a parabolic dispersion law H = P 2 /2M + U (X).…”
Section: Dw Tunnelingmentioning
confidence: 99%
“…preserves b = ∇ m × a. It is known that the linear momentum p derived from Noether's theorem is gauge-dependent [8,11]. This is a cause for concern: physical quantities should be gauge-invariant.…”
Section: Introductionmentioning
confidence: 99%
“…Tretiakov et al [16] obtain it by translating the Landau-Lifshitz equation of motion for the magnetization field m(r, t) into the language of collective coordinates q(t). Here we obtain it directly from the definition of the gauge potential (8) and magnetic field (9):…”
mentioning
confidence: 99%
“…It can be written through a surface integral of the type of dS rot m A and it is equal to S/a, multiplied by the area, on the sphere m 2 = 1, inside two trajectories, corresponding to these pairs of kinks. 33 It is clear that for a biaxial ferromagnet there are pairs of diametrically opposite trajectories (e.g., the trajectories B+ and B− in Fig. 2) corresponding to energetically equivalent but physically different kinks.…”
Section: B Topological Analysis Of Domain Wall Structurementioning
confidence: 98%