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Frequencyindependent Optical Spin Injection in Weyl Semimetals
by Yang Gao; Chong Wang; Di Xiao
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Submission summary
Authors (as registered SciPost users):  Yang Gao 
Submission information  

Preprint Link:  scipost_202211_00035v1 (pdf) 
Date submitted:  20221121 06:10 
Submitted by:  Gao, Yang 
Submitted to:  SciPost Physics 
Ontological classification  

Academic field:  Physics 
Specialties: 

Approach:  Theoretical 
Abstract
We demonstrate that in Weyl semimetals, the momentumspace helical spin texture can couple to the chirality of the Weyl node to generate a frequencyindependent optical spin injection. This frequencyindependence is rooted in the topology of the Weyl node. Since the helicity and the chirality are always locked for Weyl nodes, the injection spin from a pair of Weyl nodes always add up, implying no symmetry requirements for Weyl semimetals. Finally, we show that the photoinduced frequencyindependent injection spin is robust against multiband and lattice effect and capable of realizing alloptical magnetization switching in the THz regime.
Current status:
Reports on this Submission
Anonymous Report 1 on 2023129 (Invited Report)
 Cite as: Anonymous, Report on arXiv:scipost_202211_00035v1, delivered 20230129, doi: 10.21468/SciPost.Report.6627
Strengths
1  Addresses a problem (optical spin injection in Weyl semimetals) that, to my knowledge, had not been previously investigated in the literature.
2  Finds a noteworthy feature in that problem (frequency independence, under certain assumptions) that may stimulate further investigations, and articulates well why such a feature is desirable.
3  Clearly written, wellorganized, good balance between the material in the main text and in the appendices.
4  Numerical results illustrate in a useful way the main ideas.
5  Provides estimates in Sec. 5 that could serve as a guide for future experimental efforts.
Weaknesses
1  As stated in Sec. 2 of the manuscript, the main idea behind this work is partly inspired by Ref. [8], where the current injection in the circular photogalvanic effect was found to be frequencyindependent and quantized (under certain assumptions) in acentric Weyl semimetals, only depending on fundamental constants. The corresponding result found in the present work for spin injection is somewhat weaker, lacking the quantization aspect that was the most salient feature of the work presented in Ref. [8]. Specifically, the helicity of a Weyl node defined by Eqs. (5,6) is not quantized, as illustrated in Table 1. In that sense, the main finding of this work is less "topological" than that of Ref. [8] (which is also not truly topological, as it relies on the 2band approximation).
2  While the specific problem addressed in this work may not have been previously addressed in the literature, several theoretical works have looked at related problems in Weyl and/or Dirac semimetals. For example,
http://dx.doi.org/10.1103/PhysRevB.93.201202
https://doi.org/10.1103/PhysRevB.101.174429
https://arxiv.org/abs/2009.01388v1
https://doi.org/10.1103/PhysRevLett.126.247202
It would be useful to refer to such works in the Introduction or Conclusion[s], to help place the present work in the proper context.
Report
Of the acceptance criteria for SciPost Physics indicated in
https://scipost.org/SciPostPhys/about#criteria
my assessment is that this work does not quite meet criteria 1, 2, and 4. As for criterion 3,
"Open a new pathway in an existing or a new research direction, with clear potential for multipronged followup work."
I believe that it is at partly satisfied. However, my understanding is that it has been quite challenging to identify materials that display in a good approximation the idealized Weylsemimetal behavior, without it being masked by other "trivial" bands crossing the Fermi level. It is therefore unclear to what extent the spininjection behavior of a real "Weyl semimetal" would be dominated by the mechanism discussed in the manuscript. This also casts some doubts on the reliability of the estimates for realizing alloptical magnetization switching in the THz range.
Overall, I am unsure as to whether this submission meets the criteria of SciPost Physics, but I am confident that it does meet those of SciPost Physics Core, where it could be published.
Requested changes
1  In Fig. 1(b), shouldn't the green (spin) arrows in $h_c$ all be pointing outwards, and those in $h_v$ all be pointing inwards ("hedgehog" pattern)?
2  The caption of Fig. 1 refers to the "chirality" of light. Shouldn't it be "helicity", since it is referenced to the propagation direction?
3  Figures 2 and 3 are almost identical, the only difference being that Fig. 3 contains one additional curve in panels (b,c,d). Would it make sense to simply replace Fig. 2 with Fig. 3, and change the text accordingly? (Possibly expand the last paragraph of Sec. 4 to include some of the material in the last paragraph of Appendix C).
4  In both Figs. 2 and 3, the frequency range in panel (c) goes exactly from 0 to 3, whereas in panels (b,c) it goes slightly beyond 3, so that panels (b,d) are slightly "misaligned". Once they are aligned the tick labels above panel (b) could be removed, making the figure less busy.
5  Equation (10) is the same as (4), with an extra equality in the middle. Maybe replace Eq. (4) with (10), reducing by one the total number of equations?
6  In Appendix C, $\tau_1$ and $\tau_2$ are dummy timeintegration variables, while $\tau_0$ is the relaxation time. Would it be more clear to rename $\tau_1$ and $\tau_2$ as $t_1$ and $t_2$?
7  The relaxation time $\tau_0$ appears out of nowhere in Eq. (41). The way it is usually introduced is in the adiabatic switching on of the coupling to light. But do I understand correctly that then it should always appear in the combination $\omega+i/\tau_0$? That does not seem to be the case in the denominator of Eq. (41). Also, in the definition of $G_{ln}$ below Eq. (41) is it really just $\omega\rightarrow \omega$, or should the sign change affect $i/\tau_0$ as well?
8  Slightly inconsistent notation throughout the text concerning the traced quantity. It is variously written as $\text{Tr} \beta^\text{inj}_{ij}$ [Eq. (4)], $\text{Tr} \beta_{ij}$ [Eq. (10) and in the text above Eq. (2)], and $\text{Tr} \beta^\text{inj}$ (below Table 1). Likewise, it is written $\beta_{zz}$ in Eqs. (16,18), but $\beta_{xx}^\text{inj}$ and $\beta_{yy}^\text{inj}$ in Eq. (19).
9  The title refers to "spin injection", but the abstract talks about "injection spin", and both forms are used in the main text. Use consistently the first form?
10  In the abstract, "multiband and lattice effect" should be replaced for clarity with "multiband corrections and latticeregularization effects".
11  In the 5th line of the caption of Fig. 1, replace "velocity" with "velocity $v$", so that the symbol $v$ has been defined before it appears again three lines below. Similarly, need to define $(\Delta v)_i$ below Eq. (2).
12  Is the "static photoinduced spin magnetization" the same as the inverse Faraday effect? Is it correct that it does not require absorption/dissipation, while spin injection does?
13  Miscellaneous typos: Second line of Sec. 2: "injectin". Below Eq. (2), after $\omega_{ln}=\varepsilon_l\varepsilon_n$ there should be a comma, not a period.
14  Replace the arXiv preprint in Ref. [26] by the published article.
15  Fix capitalization in the article titles in the bibliography. For example, "taas" vs "TaAs" in Ref. [9], and many other similar issues. In bibtex, this can be achieved by placing the title entry inside double curly brackets.
16  The text could benefit from one more round of polishing revisions. Some examples: "the three plots shows" (p. 3); "the changing rate" instead of "the rate of change" (p. 3), "can be heuristically described [as] in Fig. 1(a)" (p. 3); the title of Sec. 3 would read better as "Spin injection and the helicity of a Weyl node"; "but the expression of $\beta^\text{inj}_{ii}$" ("of" $\rightarrow$ "for") (p. 5); "located at the $k_z$ axis" $\rightarrow$ "located on the $k_z$ axis" (p. 5), etc.