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Magnetism of magic-angle twisted bilayer graphene
by Javad Vahedi, Robert Peters, Ahmed Missaoui, Andreas Honecker, Guy Trambly de Laissardière
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|As Contributors:||Andreas Honecker · Guy Trambly de Laissardière · Javad Vahedi|
|Arxiv Link:||https://arxiv.org/abs/2104.10694v1 (pdf)|
|Date submitted:||2021-04-23 16:15|
|Submitted by:||Honecker, Andreas|
|Submitted to:||SciPost Physics|
We investigate magnetic instabilities in charge-neutral twisted bilayer graphene close to so-called "magic angles" using a combination of real-space Hartree-Fock and dynamical mean-field theories. In view of the large size of the unit cell close to magic angles, we examine a previously proposed rescaling that permits to mimic the same underlying flat minibands at larger twist angles. We find that localized magnetic states emerge for values of the Coulomb interaction $U$ that are significantly smaller than what would be required to render an isolated layer antiferromagnetic. However, this effect is overestimated in the rescaled system, hinting at a complex interplay of flatness of the minibands close to the Fermi level and the spatial extent of the corresponding localized states. Our findings shed new light on perspectives for experimental realization of magnetic states in charge-neutral twisted bilayer graphene.
Submission & Refereeing History
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Reports on this Submission
Anonymous Report 2 on 2021-7-20 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2104.10694v1, delivered 2021-07-20, doi: 10.21468/SciPost.Report.3265
1) Original results regarding magnetic properties of twisted bilayer graphene systems.
2) Meanfield Hubbard calculations are complemented with dynamical MF and RPA analysis.
3) Text mostly well written and clear.
1) Uncertain rescaling of U makes the comparison to single layer difficult.
In this work, magnetic properties of charge-neutral twisted bilayer
graphene systems are investigated within Hubbard model using
mean-field and dynamical mean-field appraches. In particular, the
authors find that, for systems close to magic angles, the critical
Hubbard U value to trigger antiferromagnetism insulator phase is
significantly lower than for normal bilayer and single-layer graphene.
Most of the results are obtained for "rescaled systems" to reduce
computational cost. Some of the results are checked by comparing to
non-scaled system results and shown to be consistent. However it is
found that rescaled system leads to an overestimated critical U.
I find that this is an interesting, well written and original work on
the topical subject of twisted bilayer graphene systems. I can
recommend publication of the manuscript in SciPost provided that the
authors clarifies following issues:
1) The issue of rescaling of U parameter should be (briefly)
introduced earlier in the manuscript since it raises questions about
the interpretation of results in Figs.2: should we compare the values
of U to single layer results in units of t0' or eV (I tend to think in
terms of eV)? Without knowing that U should be rescaled it leads to
2) In Fig.2b: it seems that the authors plotted the (non-twisted)
bilayer system result instead of single layer, since the critical U
value seems to be U/t=2.15. Please check the caption and the related
text on page 7. Also, are the (non-twisted) bilayer system results for AA or AB?
3) Page 9, first paragraph: I do not understand the sentence starting
with "Indeed, already single-site DMFT ...": Why does the right-hand
side of the equation has several values?
4) Although the authors find that antiferromagnetism is triggered at
lower U values, Fig.2 also shows that a clear increase in
magnetization occurs near U/t0' = 2.15. However, this effect
does not seem to be present in the DMFT results (Fig.4) which is
surprising to me. Can the authors comment on that?
As pointed out in the report section I suggest that the authors should:
1) Add a brief discussion on rescaling of U earlier in the manuscript.
2) Use the right results for single layer system in Fig.2b.
3) Correct/clarify the equation in the first paragraph on page 9.
4) Discuss the discrepancy between MFT and DMFT around Uc .
Anonymous Report 1 on 2021-6-16 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2104.10694v1, delivered 2021-06-16, doi: 10.21468/SciPost.Report.3067
Dynamical mean field theory analysis and top the static mean field theory
Introduction of the rescaled system instead of real large moire cells.
Starting from graphene, a single layer form of the graphite, two dimensional layered materials have drawn great attention in recent years, probably is the most studied systems in the last couple of years within the condensed matter and materials science community after the synthesis of graphene by mechanical exfoliation method in 2004. When the superconductivity observed in twisted bilayer system in 2018, it attracted a lot of attention from scientific community. More than 30 research groups have been studying twisted 2D layered systems since then. This is due the fact that their unusual properties of these simple systems still enrich our understanding of some fundamental physics, even might lead to some interesting applications.
This is a simple but quite interesting study; it provides a discussion about the magnetism of twisted bilayer graphene system around the magic angle of 1.08 degrees. Since, the system size is very large (Nc=11164) at this first magic angle of 1.08 degree, first rescaled system, with twist angle of 3.89 degrees and Nc=868, was introduced and discussed , so that lead a reasonable computational cost and time. Once, this established, then magnetic state of the moire system were investigated by static mean field and dynamic mean field theory based on tight binding Hamiltonian.
In conclusion, I would recommend publishing this manuscript on SciPost.
On page 4, below eq (4), order of intralayer and interlayer should be other way around.