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Coexistence of valencebond formation and topological order in the Frustrated Ferromagnetic $J_1$$J_2$ Chain
by Cliò Efthimia Agrapidis, StefanLudwig Drechsler, Jeroen van den Brink, Satoshi Nishimoto
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Submission summary
Authors (as Contributors):  Cliò Efthimia Agrapidis · Satoshi Nishimoto · Jeroen van den Brink 
Submission information  

Arxiv Link:  https://arxiv.org/abs/1806.08662v3 (pdf) 
Date submitted:  20180912 02:00 
Submitted by:  Agrapidis, Cliò Efthimia 
Submitted to:  SciPost Physics 
Ontological classification  

Academic field:  Physics 
Specialties: 

Approach:  Theoretical 
Abstract
Frustrated onedimensional (1D) magnets are known as ideal playgrounds for new exotic quantum phenomena to emerge. We consider an elementary frustrated 1D system: the spin$\frac{1}{2}$ ferromagnetic ($J_1$) Heisenberg chain with nextnearestneighbor antiferromagnetic ($J_2$) interactions. On the basis of densitymatrix renormalization group calculations we show the existence of a finite spin gap at $J_2/J_1>1/4$ and we find the ground state in this region to be a valence bond solid (VBS) with spinsinglet dimerization between thirdneighbor sites. The VBS is the consequence of spontaneous symmetry breaking through order by disorder. Quite interestingly, this VBS state has a AffleckKennedyLiebTasakitype topological order. This is the first example of a frustrated spin chain in which quantum fluctuations induce gapped topological order.
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Submission & Refereeing History
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Reports on this Submission
Anonymous Report 3 on 2018118 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1806.08662v3, delivered 20181108, doi: 10.21468/SciPost.Report.646
Strengths
The problem addressed is a nontrivial one, where for a range of parameters excitation gap above the ground state nearly vanishes. DMRG has been used effectively to show the finite but extremely small small gap. It also brings out existence of string order this nearly gapless system.
Weaknesses
Figuure 1 and 9 shows valence bond order and emergent spin1 bonds. Except for figure 1d, res of the figures are some what confusing (even though technically correct) and not illuminating. Let the authors come up with better illustrations.
Valence bond order implies existence of soliton excitation namely spinons.
I would have liked the authors to discuss them at least qualitatively. As the gap is nearly vanishing, spinons are nearly deconfined in a wide parameter region. What is the relation of the spinon with edge spinhalf excitations ?
Report
It is a good paper that confirms by powerful numerics existence of a tiny gap, string order and valence bond orders.
Requested changes
Better, non cluttered figures will make the discussed orders more transparent.
Anonymous Report 2 on 20181024 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1806.08662v3, delivered 20181024, doi: 10.21468/SciPost.Report.626
Strengths
1. Accurate DMRG numerics.
2. Attempt to uncover the tiny spin gap in the FM chain.
Weaknesses
1. Presentation needs to be improved. Since there is no restriction on space, introduction and conclusion may be expanded and many of the appendices may be integrated with the main text.
2. The authors need to provide a clear summary pf results and improvements over existing literature to put the work in proper context.
Report
May be published if the authors improve their presentation.
Requested changes
1. Expand introduction to survey existing results in greater details.
2. Appendices BF may be integrated with the main text in appropriate locations.
3. The conclusion may be expanded and the significance of the numerical results obtained may be discussed in greater details.
Author: Cliò Efthimia Agrapidis on 20181122 [id 353]
(in reply to Report 2 on 20181024)
We thank the referee for his/her comments. We here reply to them.
We integrated the appendices and expanded some parts of the text.
In the updated manuscript we change part of the presentation of the results, aiming to put them in better context.
Anonymous Report 1 on 20181012 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1806.08662v3, delivered 20181012, doi: 10.21468/SciPost.Report.611
Strengths
1 solid numerical investigation of the ferromagnetic Heisenberg chain with S=1/2 supplemented by frustrating antiferromagnetic coupling between nextnearest neighbors.
2leading edge DMRG code
3nice results on the tiny spin gaps in this system.
4 kind of VBS ordering is sorted out.
Weaknesses
1 layout: unclear distinction between main text, appendices and supplements
2 very short, cryptic explanations
3 slight overselling of the results
4 explanation of power law with exponent 2/3 unclear
5 some spelling errors in the references
Report
The authors present a solid numerical investigation
of the ferromagnetic Heisenberg chain with S=1/2
supplemented by frustrating antiferromagnetic
coupling between nextnearest neighbors. They use
a leading edge DMRG code to obtain nice results
on the tiny spin gaps in this system. In addition,
they sort out which kind of ordering occurs. It
appears to be a thirdneighbor dimerization.
All in all, the system behaves qualitatively
similar to a Haldane chain and a AKLT chain.
The topic of unexpected ordering is timely and the
results are nice so that publication in indicated.
However the presentation and the layout of the
manuscript needs some improvement:
(i)
There are a number of appendices. Are they appendices
or will they appear as supplement?
The references to them in the main text should be
consistently to appendices or to supplements.
(ii)
Often, equations and figures are quoted in the main
text which appear only in the appendices. This is
a nuisance for the readers. All material actively
used in the main text should be presented in the
main text  there are no limits on length in SciPost
anyway.
 Why is Eq. 3 on two lines?
 Which Eq. 8 is simplified?
 Why is the definition of the string order not
a proper equation with number?
(iii)
Sometimes the presentation is too short and too
cryptic. Again, no length limit constrains the authors
to improve on comprehensibility, for instance:
 What is meant by "arbitrary set of valence bonds"
(end of page 3)?
 Which "twofold degeneracy" is referred to after Eq. (3)?
 Where does the formula 42(delta mod 2) come from?
(line 1 on page 5)
(iv)
Understandably, the authors want to sell their results.
But I think they exaggerate slightly:
 Why is the phenomenon "order by disorder"?
That term usually refers to classical degeneracy lifted
by fluctuations. I do not see this here. And
if it were, it were not the "first example"
as stated in the abstract, see Haldane chain
or MajumdarGhosh chain.
 Clearly, the system shows long range string order.
But why is this topological? What is the relevant manifold,
the fibre bundle and the topological invariant of this
topological order? If the authors insist on the term
"topological" these issues should be discussed.
(v)
In the Introduction, a number of compounds is given
which potentially realize the investigated chain.
The reader will wonder what one can learn from the
theoretical results for these compounds. So it should
be discussed briefly which messages for the compounds
can be taken from the theoretical results.
(vi)
The dependence of the spin gap on J_3' with a power law
with exponent 2/3 is very interesting.
But the references quoted treat the massless case
without gap in absence of VBS. Hence their results
do not apply here.
I presume the exponent can rather be explained by
the binding of two solitons. The authors may consider
this scenario, see for instance Uhrig et al. EPJB
7, 67 (1999).
(vii)
There are spelling errors in the references, see e.g.
Refs. 6, 21 and 24.
Requested changes
1Please address AG consistently as appendices or as supplement.
In the latter case, they should be submitted as separate file.
2Eqs and Figs. quoted in the main text should be given in the main text.
3Too short and cryptic statements should be expanded, see examples in Report
4Avoid the expression "order by disorder". It is in appropriate here.
5The last sentence of the abstract should be omitted.
6Either avoid the term "topological order" for string order or explain
the topological aspect in more detail.
7Briefly mention any relevance of the theoretical results for the
compounds quoted in the beginning.
8Explain the exponent 2/3 for gapped solitons, not gapless solitons.
9Check list of references for spelling errors.
Author: Cliò Efthimia Agrapidis on 20181122 [id 354]
(in reply to Report 1 on 20181012)
We thank the referee for his/her comments. We here reply to them.
(i) In the new version, we changed the main text to refer to the appendices as, for example, App. A. We now moved
most of the appendixes to the main text, apps. BG.
(ii) We now moved materials addressed in the main text to the main text itself. We put eq. 3 in one line and the simplification of the string order parameter is presented as a proper equation with number. The reference to eq. (8) in the main text has been corrected.
(iii)
The statement "arbitrary set of valence bonds" refers to the possibility that the VB might form in different directions, as shown in fig. 1(b). We added further explanations about this in the main text.
We refer to the twofold degeneracy due to the dimerization: because of the particular boundary conditions we use (explained in the methods section), the degeneracy is lifted with OBC.
When $\delta$ is odd the period is 2. It is clear for $\delta=1$ because a dimerized and an undimerized bond appear alternately along the $J_1$ chain. For $\delta>1$ it may be helpful to consider the system within the topologically equivalent ladder geometry. In this case, as seen in Fig.1(c) the translation symmetry along the $J_2$ chains is not broken but the mirror symmetry between two $J_2$ chains is broken. This leads to a period of 2 along the $J_1$ chain. Whereas for even $\delta$, as seen in Fig.9(b), the translation symmetry is broken along the $J_2$ chains with twofold structure and also the mirror symmetry between two $J_2$ chains is broken. Thus, the period is $2\times2=4$ along the $J_1$ chain. We added a more detailed explanation about this in the main text.
(iv)
Our system is a geometrically frustrated chain: its classical ground state is highly degenerate, the quantum fluctuations lift this degeneracy with the formation of FM dimers and valence bonds. As the referee points out, the MajumdarGhosh chain is a consequence of order by disorder but the presence of topological order has not been discussed yet. We expanded the text in the manuscript on this point.
The nonlocal string order parameter is a wellused quantity to detect the AKLT or Haldane state as a topological state. We appreciate the point raised by the referee and in order to further prove the topological nature of the AKLTlike VBS (Haldane) state appearing in this model, we have computed the entanglement spectra for different values of $\alpha$ to show the existence of fractionalized edge excitations: they clearly show a QPT from a trivial state (FM state) to a nontrivial one ($\mathcal D_3$VBS state). We attach a figure showing (a) how the system is cut and (b) the resulting ES as a funtion of $\alpha$. We added these results in the main text of the manuscript.
(v) We now discuss the implications of our results on the cited compounds in the conclusions.
(vi) We agree with the suggestion. Since our system is massive, it should be explained by binding of two solitons. We replaced our previous citation about the exponent by Uhrig et al. EPJB 7, 67 (1999). We also added some more explanations about this issue.
(vii) We carefully went through the references and corrected the spelling mistakes.
Author: Cliò Efthimia Agrapidis on 20181122 [id 352]
(in reply to Report 3 on 20181108)We thank the referee for his/her comments. We here reply to them.
We revised the figures to improve the presentation of the different states.
Thank you for the interesting question to improve the manuscript. As the referee suggests, spinons are nearly deconfined. In Fig.6(a) a spinon is created at the system edges as an edge spinhalf excitation. Typically, the Friedel oscillation decays quickly (decay length is of the order of $1$) from the edges in a gapped system. If the edge spinhalf is completely free, the decay length is 0. However, in our system it decays very slowly and the amplitude seems to be finite even around the system center for $L=600$. This is also consistent with an exponential decay of the spinspin correlation with very large decay length, $\xi\sim50$ ($\alpha\sim0.6$) at minimum. We added this explanation in the main text.