SciPost Submission Page
Half-wormhole in SYK with one time point
by Baur Mukhametzhanov
This is not the latest submitted version.
This Submission thread is now published as
Submission summary
| Authors (as registered SciPost users): | Baurzhan Mukhametzhanov |
| Submission information | |
|---|---|
| Preprint Link: | https://arxiv.org/abs/2105.08207v3 (pdf) |
| Date submitted: | 2021-07-21 23:00 |
| Submitted by: | Mukhametzhanov, Baurzhan |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
|
| Approach: | Theoretical |
Abstract
In this note we study the SYK model with one time point, recently considered by Saad, Shenker, Stanford, and Yao. Working in a collective field description, they derived a remarkable identity: the square of the partition function with fixed couplings is well approximated by a "wormhole" saddle plus a "half-wormhole" saddle. It explains factorization of decoupled systems. Here, we derive an explicit formula for the half-wormhole contribution. It is expressed through a hyperpfaffian of the tensor of SYK couplings. We then develop a perturbative expansion around the half-wormhole saddle. This expansion truncates at a finite order and gives the exact answer. The last term in the perturbative expansion turns out to coincide with the wormhole contribution. In this sense the wormhole saddle in this model does not need to be added separately, but instead can be viewed as a large fluctuation around the half-wormhole.
Current status:
Reports on this Submission
Report #3 by Anonymous (Referee 3) on 2021-9-26 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2105.08207v3, delivered 2021-09-26, doi: 10.21468/SciPost.Report.3573
Report
This paper presents an interesting result in the context of a recent work by Saad-Shenker-Stanford-Yao (SSSY). The main result is an exact computation for the partition function $z^2$ with two boundaries in the SYK model at one point in time. This takes the form of a perturbative expansion that truncates at finite order. It is shown that the wormhole can be seen as a fluctuation of the half-wormhole contribution, so that it should not be included separately. The result is significant and meets the criteria for publication in SciPost Physics. I recommend the paper for publication if the following minor points can be addressed:
1. The terminology "half-wormhole contribution" is a bit confusing as it could equally refer to the "unlinked half-wormhole contribution" which is the RHS of (3.13) in SSSY. Then it's obvious that the wormhole should not be included (as it would contradict factorization). Of course, the present paper is about the "linked half-wormhole contribution" which appears in the LHS of (3.13). Then it's a non-trivial and interesting result that the wormhole should not be included (as it appears as a fluctuation of the linked contribution, as the author has shown). It would be great to perhaps add a few words about this.
2. I also second another referee about the perturbative expansion (43). The fact that this is actually an expansion in 1/N (only for a typical realization) could be explained better.
Report #2 by Anonymous (Referee 2) on 2021-9-16 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2105.08207v3, delivered 2021-09-15, doi: 10.21468/SciPost.Report.3536
Report
This work is a future development of a previous work by Saad, Shenker, Stanford and Yao about resolving the factorization puzzle in the SYK model with one time point. The main result is the observation that the wormhole saddle can be obtained as a truncation of a perturbative expansion along the half wormhole saddle. This is explained clearly in equation 43 in the paper.
One question I had is it is not clear to me that this is perturbative expansion in 1/N, which is what usually do in a large N system. From the discussion below equation 43, it seems that it is a perturbative expansion in J^2. Maybe the author can clarify this point a little bit.
There are some minor presentation issues of the paper, such as the lack of definition of sin(A) in equation A and how to go from equation 29 to 30.
Report #1 by Anonymous (Referee 1) on 2021-8-29 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2105.08207v3, delivered 2021-08-29, doi: 10.21468/SciPost.Report.3459
Report
This paper studies the "wormhole" and "half-wormhole" saddles in the SYK model with one time point. The topic of the paper is interesting and the results are new and well written. Therefore, I recommend for publication in SciPost Physics once the author addresses the following points. \\
$\bullet$ There is no small coupling constant for $\Phi(\sigma)$ in (22), so it's not clear in what sense these "saddles" are dominant and fluctuations around these saddles are suppressed. It would be good to explain this point more. \\
$\bullet$ In section~4.2, the author states that the approximation (23) is valid for a typical realization of the couplings. It is needed to describe the criteria for this 'typicalnes' of the couplings. More concretely, in section~4.2, it is shown that $\langle {\rm Error} \rangle^2$ is small for large $N$, but this does not mean the "Error" itself is small. It would be good to explain for what type of configuration of the couplings, the "Error" itself is indeed small. \\
$\bullet$ The only reason that we expect the ordinary (one-dimensional) SYK model is related to AdS$_2$ gravity is the symmetry breaking pattern of $SL(2,R)$. It's desirable to clarify why this type of reduction to one time point is still meaningful for gravitational theory. \\
Author: Baurzhan Mukhametzhanov on 2021-09-03 [id 1732]
(in reply to Report 1 on 2021-08-29)
I would like to thank the referee for reading the manuscript and address the raised issues:
1),2) The first two questions are related, so I'll address them together. Indeed, as explained in the beginning of section 4.2, the approximation (23) is valid only for a ''typical'' realization of the couplings. This is expressed mathematically, by computing $\langle Error^2 \rangle$ and showing it is suppressed at large $N$. This is what is meant by the couplings being ''typical''.
As pointed out by the referee, this doesn't mean that Error itself for fixed couplings is small. This point is made in the first two sentences of section 4.2. In fact, by choosing some very special set of couplings it is possible to make $z^2$ deviate substantially from the approximation (23). Nevertheless, for most couplings, or on average, the Error is small.
I agree with referee's sentiment that it would be nice to know for what type of couplings the Error itself is small, but I do not have anything to add on this point at the moment.
3) A relation between SYK with one time point and some putative 1d gravity is purely speculative. At the moment, the only reason one might think it might have anything to do with a gravity theory, is that it has features that are similar to (one-dimensional) SYK. However, having gained some intuition in the toy model, one could look for a similar mechanism of factorization in theories that are known to have bulk duals, e.g. SYK, matrix models or higher dimensional QFTs.
I can make these points clearer in the paper, if necessary.
Anonymous on 2021-10-30 [id 1890]
(in reply to Baurzhan Mukhametzhanov on 2021-09-03 [id 1732])Sufficiently addressed the points I raised. Good for publication.
Author: Baurzhan Mukhametzhanov on 2021-09-22 [id 1773]
(in reply to Report 2 on 2021-09-16)I would like to thank the referee for reading the manuscript and comments and address his/her questions:
1) Indeed, the expansion in eq.(43) for a given fixed set of couplings is not an expansion at large $N$ in the usual sense for any fixed set of couplings. One can happen to choose a particularly bad set of couplings for which $\Phi_k$ are not suppressed as we go to higher orders $k$.
Instead, as in the paper of Saad, Shenker, Stanford and Yao, it is an expansion at large $N$ for a ''typical'' choice of couplings. This is explained in eqs. (50), (51) (or the exact result (46)) and the discussion around them. So if one randomly chooses a fixed set of couplings, with high probability the expansion (43) would be an expansion at large $N$. So it is not a usual Taylor series at large $N$. But for most randomly chosen fixed set of couplings it is an expansion at large $N$.
2) By definition $sgn(A)$ is the sign of the permutation $A_1...A_p$, where $A_j = \left( a_1^{(j)}<...< a_q^{(j)} \right) $ is an ordered $q$-subset (see (4)).
I can add this definition as well as a clarification about eqs. (29), (30) in the new version of the draft.