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DMRG study of strongly interacting $\mathbb{Z}_2$ flatbands: a toy model inspired by twisted bilayer graphene
by P. Myles Eugenio, Ceren B. Dağ
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Submission summary
Authors (as registered SciPost users):  Paul Eugenio 
Submission information  

Preprint Link:  https://arxiv.org/abs/2004.10363v1 (pdf) 
Date submitted:  20200501 02:00 
Submitted by:  Eugenio, Paul 
Submitted to:  SciPost Physics 
Ontological classification  

Academic field:  Physics 
Specialties: 

Approaches:  Theoretical, Computational 
Abstract
Strong interactions between electrons occupying bands of opposite (or like) topological quantum numbers (Chern$=\pm1$), and with flat dispersion, are studied by using lowest Landau level (LLL) wavefunctions. More precisely, we determine the ground states for two scenarios at halffilling: (i) LLL's with opposite sign of magnetic field, and therefore opposite Chern number; and (ii) LLL's with the same magnetic field. In the first scenario  which we argue to be a toy model inspired by the chirally symmetric continuum model for twisted bilayer graphene  the opposite Chern LLL's are Kramer pairs, and thus there exists timereversal symmetry ($\mathbb{Z}_2$). Turning on repulsive interactions drives the system to spontaneously break timereversal symmetry  a quantum anomalous Hall state described by one particle per LLL orbital, either all positive Chern $++\cdots+>$ or all negative $\cdots>$. If instead, interactions are taken between electrons of likeChern number, the ground state is an $SU(2)$ ferromagnet, with total spin pointing along an arbitrary direction, as with the $\nu=1$ spin$\frac{1}{2}$ quantum Hall ferromagnet. The ground states and some of their excitations for both of these scenarios are argued analytically, and further complimented by density matrix renormalization group (DMRG) and exact diagonalization.
Current status:
Reports on this Submission
Anonymous Report 1 on 2020613 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2004.10363v1, delivered 20200613, doi: 10.21468/SciPost.Report.1757
Strengths
1. The given toy model for strongly interacting oppositeChern ﬂat bands is straightforward.
2. A connection between the excited states and 1D Isingtype spin physics is interesting.
3. A useful information about numerical approach to quantum Hall system is provided.
Weaknesses
1. The numerical results are rather obvious.
2. The discussion about numerical results is insufficient.
3. There is room for improvement on the presentation.
Report
The authors provided a simple model to capture the essential physics of two strongly interacting ﬂat bands for the cases that the bands have identical (spin1/2 QH) or opposite ($\mathbb{Z}_2$) Chern number. By studying the model numerically with a cylinder geometry, it was found that the gap to the ﬁrst excited states remains finite for the $\mathbb{Z}_2$ case and it is significantly shrunk for the spin1/2 QH case. Although the obtained results are rather obvious, the used numerical approaches would be useful information for future studies of quantum Hall system. Furthermore, the discussion on the nature of the excited states, especially a connection to 1D Isingtype spin physics, is interesting. Therefore, the contents of this manuscript seem to be enough for the publication in SciPost. However, I think that the discussion about numerical results is insufficient and ambiguous descriptions are seen in the presentation. Hence, I cannot recommend the publication in the present form. Then, I would like to request the improvement of the manuscript with addressing the following questions/suggestions.
 Is the number of LLL orbitals counted like $N=L_xL_y/(2\pi)$? If yes, how can one take $N=4, 6, 8,$ …, as shown in FIG.3 and FIG.4? Namely, what is the relation between $N$ and $L_x$?
 What is the definition of gap? Is it $\Delta E=E_1E_0$? Also, does the singleparticle gap provide the same result in the $\mathbb{Z}_2$ case or not? It would be a useful information for DMRG calculation.
 It is unclear how the parameters $l_s$, $l_B$ are chosen in FIG.3 and FIG.4. For example, the used choice of $l_B=1$ corresponds to $B=1$. Does it fulfill the condition that the gap between Landau levels is much larger than the interaction strength?
 In FIG.3, why the gap is larger for larger $L_y$, even though the gap between Landau levels typically depends only on $B$?
Related to the above question, the data only for two circumferences may be not enough to confirm the saturation of the gap in the thermodynamic limit. If possible, it would be better to add one more data for another $L_y$ even if it is smaller than $L_y=15$.
 In FIG.3, one may naively think that the gap for the shortrange contactlike interaction is larger than that for the screened Coulomb interaction but the result is opposite. Is the limit $l_s\to0$ of $V_{sc}$ quantitatively connected to $V_\delta$?
 Is the caption of FIG.4 correct? What does "plotted as $(\Delta E)^{−1}$" mean?
The horizontal axis of FIG.4 should start from $1/N=0$. If possible, it would be better to discuss the gap in the thermodynamic limit.
 Which parameter value is used in FIG.5 and FIG.6?
 In FIG.5 and FIG. 6 the data for $L_y=2$ seems to deviate from the systematic size dependence. Is a periodic boundary indeed applied in the ydirection for $L_y=2$, namely, is the hopping taken twice?
 In FIG.7, it would be helpful for readers to put numbers in the color bar to estimate how strongly a spin is localized.
 The accuracy of DMRG should be written, even if the discarded weight is negligible.
Requested changes
1. The parameters and quantities should be clearly defined.
2. The reason why the used parameters were chosen should be clearly written.
2. More discussion about the interpretation of numerical results, especially for FIG.3 and FIG.4, should be added.
3. The presentation (including the caption) of some figures should be improved.
Author: Paul Eugenio on 20200916 [id 972]
(in reply to Report 1 on 20200613)Please see the attached pdf.
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sciPost_replyLetter.docx.pdf