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How a skyrmion can appear both massive and massless
by Xiaofan Wu, Oleg Tchernyshyov
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|Authors (as registered SciPost users):||Oleg Tchernyshyov · Xiaofan Wu|
|Preprint Link:||https://arxiv.org/abs/2201.08519v3 (pdf)|
|Date submitted:||2022-02-01 03:37|
|Submitted by:||Wu, Xiaofan|
|Submitted to:||SciPost Physics|
We explain how a ferromagnetic skyrmion can appear massive in some experiments and massless in others. The answer depends on the nature of the driving force. Two illuminating cases are the Zeeman coupling to a nonuniform magnetic field and the adiabatic spin-transfer torque from an electric current.
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- Cite as: Anonymous, Report on arXiv:2201.08519v3, delivered 2022-04-04, doi: 10.21468/SciPost.Report.4858
This is a very interesting article, where a fresh idea how to “visualize” dynamics of magnetic skyrmion. Concretely, dynamics of the guiding center (GCD) and Larmor dynamics (LD), naturally associated with two lowest magnon modes upon the skyrmion, are described here by two inertia-free particles. Then two possible regimes of forced motion are found, one for GCD + LD and one for GCD only. This observation is useful step to understanding of the general picture of skyrmion dynamics that is obviously of a great interest for both general magnetics and applications. For me, this article is warrant for publication in highest-rating journal like Sci. Post Phys.
i. But I have one technical question concerning “a modest generalization of Thiele’s approach”. It seems to me, Eq. (27) contains a controversy: for 2D topological solitons, any form of \phi(r) has a singular point. The distribution of magnetization vector is free of singularities if and only if this singular point for \phi(r-r_2) coincide with the values of r_1, where theta = 0 or theta = pi. Thus, to be consistent, the ansatz (27) should include some complicated constrain that is not discussed here. At least, the coordinates r_1 and r_2 are not completely independent. Of course, the coefficients F_ij can be found at r_1 = r_2, as it is done in Eq. (31), but for general case r_1 \neq r_2 the above singularity manifest itself.
ii. On the best of my knowledge, the problem of the mass for 2D solitons, both topological and non-topological, was first considered in the article [B. A. Ivanov and V. A. Stephanovich, Two-dimensional soliton dynamics in ferromagnets, Phys. Letters A4, 89 (1989).]. In this article, no driving force was considered at all; and the soliton velocity was found to be the cause of deformation. The mass was found through the kinetic energy. How it can be compared with that in the referred article?
It seems to me, the answering of these two questions can be useful for potential readers. Concerning (i), some minor explanation can be done. The detailed discussion of the item (ii) is not mandatory, but could be very useful. After doing these changes, the article can be published in Sci. Post Phys.
- Cite as: Anonymous, Report on arXiv:2201.08519v3, delivered 2022-03-30, doi: 10.21468/SciPost.Report.4826
The paper is written clearly in a good pedagogical manner.
The paper does not add much to the already existing discussion.
This paper contributes to the discussion about the mass of a ferromagnetic skyrmion. In terms of the collective coordinates, the dynamics of a finite-size skyrmion is reduced to the dynamics of a point -- skyrmion center. It is already well known that the dynamics of the skyrmion center depends on its definition:
(i) If the skyrmion center is defined as the first moment of the topological charge, then the dynamics is massless.
(ii) If the skyrmion center is defined in a manner that implies the coupling of the translational mode with the higher magnon modes, then the dynamics can be massive. For example, the skyrmion center can be defined as the first moment of the $m_z$-component.
The new finding of this paper is that in case (ii) the skyrmion dynamics can be massive or massless depending on the driving force. In addition, the paper is written in a good pedagogical manner with the use of mechanical analogies. Based on this I support publishing in SciPost Physics.
However, I have a number of observations:
1. The abstract is written in a misleading manner. The main statement is that massive or massless behavior depends on the driving force. However, it is not written that this statement refers to case (ii). I suggest a reformulation of the abstract.
2. The meaning of the quantity $G$ in (23) is not explained.
3. I think that the derivation of (35) should be explained in more detail. For me it is not obvious, how (35) follows from (34).
The abstract should be reformulated in a not misleading manner.