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Coherent forward scattering as a robust probe of multifractality in critical disordered media
by Maxime Martinez, Gabriel Lemarié, Bertrand Georgeot, Christian Miniatura, Olivier Giraud
This Submission thread is now published as
Submission summary
Authors (as registered SciPost users): | Olivier Giraud |
Submission information | |
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Preprint Link: | scipost_202210_00061v1 (pdf) |
Date accepted: | Dec. 22, 2022 |
Date submitted: | Oct. 11, 2022, 4:54 p.m. |
Submitted by: | Giraud, Olivier |
Submitted to: | SciPost Physics |
Ontological classification | |
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Academic field: | Physics |
Specialties: |
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Approach: | Theoretical |
Abstract
We study coherent forward scattering (CFS) in critical disordered systems, whose eigenstates are multifractals. We give general and simple arguments that make it possible to fully characterize the dynamics of the shape and height of the CFS peak. We show that the dynamics is governed by multifractal dimensions $D_1$ and $D_2$, which suggests that CFS could be used as an experimental probe for quantum multifractality. Our predictions are universal and numerically verified in three paradigmatic models of quantum multifractality: Power-law Random Banded Matrices (PRBM), the Ruijsenaars-Schneider ensembles (RS), and the three-dimensional kicked-rotor (3DKR). In the strong multifractal regime, we show analytically that these universal predictions exactly coincide with results from standard perturbation theory applied to the PRBM and RS models.
Published as SciPost Phys. 14, 057 (2023)
Reports on this Submission
Report #2 by Anonymous (Referee 2) on 2022-11-20 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202210_00061v1, delivered 2022-11-20, doi: 10.21468/SciPost.Report.6163
Strengths
2-new simulation of system, with perspective for experimental realization
3-well written
Weaknesses
Report
I think the manuscript reports on interesting work. It is well written, provides interesting details to their previous Letter, Ref. [46], and extends numerical studies in the latter to two additional models for the Anderson localization transition. Specifically, the detailed numerical analysis of the 3d kicked rotor seems interesting for possible future experiments. I, therefore, support publication of the manuscript in its present form. A minor remark is that I would appreciate if the authors could comment on the statistics of the forward peak? I.e. how do fluctuations of the peak height in the critical state compare to those in the Anderson localized regime?
Report #1 by Vladimir Kravtsov (Referee 1) on 2022-11-7 (Invited Report)
- Cite as: Vladimir Kravtsov, Report on arXiv:scipost_202210_00061v1, delivered 2022-11-07, doi: 10.21468/SciPost.Report.6081
Strengths
1- Very well written paper 2-Detailed derivation of main results 3-Comparison of numerics on three different models, both Hamiltonian (PLBRM) and Floquet (kick-rotor models), confirms the main results
Weaknesses
1- significant overlap with the earlier short paper of the same authors Ref.[46]. For an expert the derivations of results in this paper is sufficient to understand their validity and significance. The present manuscript does not add much to understanding of the phenomenon.
Report
In view of a great current interest to non-ergodicity of extended states in quantum disordered systems with and without interaction, this study (as well as Ref.[46]) is a significant progress in the field with a potential to observation of the effects in real experiments.
I do not have doubts about validity of the results and their significance. The only reservation I have is that the most interesting and fundamental findings are already communicated by authors in Ref.[46].
On the other hand, many of the important papers on the subject of non-ergodicity of extended states in disordered quantum systems are published in SciPost Physics. So, this paper may be a good addition to already existent collection in SciPost Physics. I think it will have an impact just because it is easy to read, also for non-specialists.
In view of this I recommend to publish the paper in its present form.