SciPost Submission Page
A symmetry algebra in double-scaled SYK
by Henry W. Lin, Douglas Stanford
Submission summary
| Authors (as registered SciPost users): | Henry W. Lin |
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| Preprint Link: | https://arxiv.org/abs/2307.15725v1 (pdf) |
| Date accepted: | Nov. 27, 2023 |
| Date submitted: | Aug. 10, 2023, 6:14 p.m. |
| Submitted by: | Henry W. Lin |
| Submitted to: | SciPost Physics |
| Ontological classification | |
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| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
The double-scaled limit of the Sachdev-Ye-Kitaev (SYK) model takes the number of fermions and their interaction number to infinity in a coordinated way. In this limit, two entangled copies of the SYK model have a bulk description of sorts known as the "chord Hilbert space." We analyze a symmetry algebra acting on this Hilbert space, generated by the two Hamiltonians together with a two-sided operator known as the chord number. This algebra is a deformation of the JT gravitational algebra, and it contains a subalgebra that is a deformation of the $\mathfrak{sl}_2$ near-horizon symmetries. The subalgebra has finite-dimensional unitary representations corresponding to matter moving around in a discrete Einstein-Rosen bridge. In a semiclassical limit the discreteness disappears and the subalgebra simplifies to $\mathfrak{sl}_2$, but with a non-standard action on the boundary time coordinate. One can make the action of $\mathfrak{sl}_2$ algebra more standard at the cost of extending the boundary circle to include some "fake" portions. Such fake portions also accommodate certain subtle states that survive the semi-classical limit, despite oscillating on the scale of discreteness. We discuss applications of this algebra, including sub-maximal chaos, the traversable wormhole protocol, and a two-sided OPE.
Published as SciPost Phys. 15, 234 (2023)
Reports on this Submission
Report #2 by Daniel Harlow (Referee 2) on 2023-11-17 (Invited Report)
- Cite as: Daniel Harlow, Report on arXiv:2307.15725v1, delivered 2023-11-17, doi: 10.21468/SciPost.Report.8143
Report
Report #1 by Anonymous (Referee 1) on 2023-9-19 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2307.15725v1, delivered 2023-09-19, doi: 10.21468/SciPost.Report.7841
Strengths
1- The paper is concerned with exploring important questions related to the bulk dual of the SYK model at finite temperature, and derives a concrete result about the sub-maximal chaos exponent.
2- It generalizes the near horizon symmetries of JT gravity.
Weaknesses
Report
On way to the above result they discovered a symmetry sub-algebra of the chord algebra that reduces to the SL2 algebra of near horizon symmetries, in the limit λ → 0, at finite temperature. This result would imply a maximal Lyapunov exponent! The puzzle is resolved by demonstrating that the bulk dual of the large p SYK model is defined on an extended “fake” disk, on which the SL2 has a natural action, leading to a sub-maximal Lyapunov exponent.
The chord (bi)-algebra at finite λ and its representation theory is discussed in detail. They find that the symmetry sub-algebra has finite dimensional unitary representations related to worm holes with an integral chord number.
The paper is very well written and discusses the chord Hilbert space and its operator algebra in detail and raises a host of interesting questions related to a discrete generalization of the geometric JT gravity and its symmetry algebra and generalization to higher dimensions.
Requested changes
None
Author: Henry Lin on 2023-12-06 [id 4173]
(in reply to Report 2 by Daniel Harlow on 2023-11-17)Hi Daniel, in response to your question: no, we did not find any mistakes in the canonical texts on finite p SYK. We just give a "geometric" interpretation of some pieces of the 4-pt function of finite p SYK. Since we have a bulk Hilbert space formalism, we can say more clearly what (a subset of) the states that are produced when we collide 2 particles, etc. In the previous path integral approaches to the 4-pt function, one could try to interpret some terms as coming from "states" in some intermediate channel but it wasn't totally clear how to describe these states as elements in a Hilbert space.