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Abelian and non-abelian symmetries in infinite projected entangled pair states
by Claudius Hubig
This is not the current version.
|As Contributors:||Claudius Hubig|
|Submitted by:||Hubig, Claudius|
|Submitted to:||SciPost Physics|
|Subject area:||Condensed Matter Physics - Theory|
We show how to implement arbitrary abelian and non-abelian symmetries in the setting of infinite projected entangled pair states on the two-dimensional square lattice. We observe a large computational speed-up obtained through the increased sparsity and reduced tensor sizes; easily allowing bond dimensions $D = 10$ in the square lattice Heisenberg model at computational effort comparable to calculations at $D = 6$ without symmetries. We also find that absent spontaneous symmetry breaking, implementing a symmetry does not negatively affect the representative power of the state and leads to identical ground-state energies. Furthermore, we point out how we can use symmetry implementations to detect such spontaneous symmetry breaking.
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Reports on this Submission
Anonymous Report 2 on 2018-10-15 Invited Report
1-written in good and clear language
2-some interesting results
1-Seems to aim to be a method paper, but doesn't explain the method clearly enough for those that do not already know a great deal about it
2-main message not clear
I think the paper should probably be published, eventually, but while reading it I was struggling a bit to figure out what the main message, or point of the paper is. From the abstract and introduction, I expected it to be a method paper, explaining the method and then applying it to some examples. However, I do not find the methods to be very clearly explained. The last part of the paper makes it sound a bit like the detection of spontaneous symmetry breaking is the main point. I think maybe the paper should be a method paper, but in this case I would recommend some modifications that clarify the method to those that don't know it. I make some suggestions and comments below on this point.
In the discussion of the Kagome lattice, I believe there are some more works that could and probably should be cited. The work of He et al (Phys. Rev. X 7, 031020 (2017)) for example, seems to me to be relevant.
1-Eq. (2) introduces the $c_i^\gamma$ tensor, but I find it hard from the discussion to understand (without prior knowledge) what they are. It would be good to clarify a bit better what they are, for example by taking a simple example for U(1) and SU(2). In particular, I'm not sure the definition given in terms of addition rule is very clear.
2-The abbreviation FFU used in caption of Fig. 2 is never defined. The same is true about CTM used in several places.
3-I would suggest to define D explicitly, for example in the context of Fig. 1. Of course, people that know will know, but it's good to actually spell it out somewhere.
4-The definition of the remover tensor R is not fully clear. I would be more explicit and maybe give an example.
5-There have been many papers, as cited by the author, on implementing SU(2) symmetries. It would be useful to be even more explicit about what is different or new in the case if iPEPS, as presented in this work.
Anonymous Report 1 on 2018-10-2 Invited Report
The paper by Claudius Hubig on on "Abelian
and non-abelian symmetries in infinite projected entangled
pair states" is a well-presented and balanced study of the application of
SU(2) symmetries in the 2D-iPEPS context; therefore I recommend
publication of this article in SciPost, after the following
comments have been clearly addressed in the paper.
It may have escaped the author that an SU(2) iPEPS study was
already also performed by Liu et al. on the spin-1 Kagome
Heisenberg antiferromagnet [see PRB 91, 060403(R) (2015)].
There (also) comparable ground state energies were observed,
with and without SU(2) symmetries at sufficiently large D.
Fig. 5 shows data for U(1) and SU(2) on the Kagome lattice,
both apparently from the present algorithm based on a square
lattice tensor network representation of the Kagome lattice.
The data appears to converge to significantly different values
for larger D, which appears to contradict the sentence in the
abstract: "We also find that [in the absence of spontaneous
symmetry breaking] implementing a symmetry does not negatively
affect the representative power of the state and leads to
identical ground-state energies."
What does the author mean by "avoiding inadequate truncations"?
While truncating into degenerate multiplets leads to error
at insufficient D, if an algorithm is deterministic, it should
converge to the same result, once D is large enough.
But again, the data in Fig. 5 for U(1) and SU(2) converges
to significantly different values. So what does this imply
on the reliability of the implemented iPEPS algorithm itself,
if the ground state depends on the history in imaginary time
It appears to me that "inadequate truncations" leads to
loss of (some generalized) "orthonormality" in the tensor network, i.e.
the deterioration of the conditioning of the environment while
truncating. I was under the impression that gauge fixing
was designed to deal with this problem. Apparently not?
It surprises me, that the energy of the U(1) data in Fig. 5
lies that far above the SU(2) data, throughout, for all D:
one would have expected that for small(er) D, the U(1) or
no-symmetry iPEPS would be superior because for the same D,
it has a larger variational parameter space available.
Why isn't this so?
The data for `None' in Fig. 5 is barely visible hidden
underneath the other symbols; one may mistake the red
horizontal line for this data.