ASEP/DSSYK duality and strange correlator
Pith reviewed 2026-06-26 20:14 UTC · model grok-4.3
The pith
The moment of the DSSYK transfer matrix equals an overlap between the ASEP stationary state and a product state.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We show that the moment of the transfer matrix of the double scaled SYK model is written as an overlap between the stationary state of ASEP and a product state. We argue that this overlap is an analogue of the strange correlator appearing in the correspondence between the Levin-Wen string-net model and the Turaev-Viro state sum.
What carries the argument
The overlap between the stationary state of the asymmetric simple exclusion process (ASEP) and a product state, which the paper identifies as the analogue of the strange correlator.
If this is right
- Moments of the DSSYK transfer matrix become computable by solving the stationary distribution of the ASEP.
- The strange-correlator analogy supplies a concrete dictionary between DSSYK observables and quantities already studied in topological state-sum models.
- The duality furnishes a probabilistic interpretation for certain correlation functions that appear in the double-scaled SYK model.
- Known exact solutions and integrability techniques for the ASEP can be imported to evaluate SYK quantities that were previously accessible only numerically or via random-matrix methods.
Where Pith is reading between the lines
- The mapping suggests that time-evolution operators in the SYK model may admit a hidden representation as Markov chains on particle configurations.
- If the analogy to the strange correlator is tight, then DSSYK partition functions could inherit topological invariance properties under certain deformations.
- One could test the duality by comparing the large-N scaling of the ASEP overlap against known SYK moment asymptotics.
Load-bearing premise
The assumption that the identified overlap in the ASEP-DSSYK mapping functions as the direct analogue of the strange correlator in the Levin-Wen string-net / Turaev-Viro correspondence.
What would settle it
An explicit calculation of the ASEP overlap for finite system size that fails to reproduce the corresponding DSSYK transfer-matrix moment at the same parameters would falsify the claimed equality.
read the original abstract
We show that the moment of the transfer matrix of the double scaled SYK model is written as an overlap between the stationary state of ASEP (asymmetric simple exclusion process) and a product state. We argue that this overlap is an analogue of the strange correlator appearing in the correspondence between the Levin-Wen string-net model and the Turaev-Viro state sum.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims to show that a moment of the transfer matrix of the double-scaled SYK (DSSYK) model equals an overlap between the stationary state of the asymmetric simple exclusion process (ASEP) and a product state. It further argues that this overlap is an analogue of the strange correlator in the Levin-Wen string-net model / Turaev-Viro state-sum correspondence.
Significance. If the overlap identity is rigorously derived and the analogy to the strange correlator is substantiated with explicit checks, the result would establish a concrete link between the DSSYK model, an integrable classical stochastic process (ASEP), and topological invariants. This could provide new computational tools or interpretive bridges in the study of quantum chaos and anyonic systems. The overlap identity itself, if verified, would be a non-trivial result independent of the interpretive claim.
major comments (2)
- [Abstract] Abstract: the central claim that a moment of the DSSYK transfer matrix equals the ASEP overlap is asserted without derivation, intermediate steps, explicit equations, or verification against the models' definitions, so the equality cannot be checked from the manuscript's content.
- [Abstract] Abstract (final sentence): the argument that the identified overlap functions as the direct analogue of the strange correlator requires explicit verification that it reproduces key properties (invariance under local moves, relation to a topological invariant, or matching under anyon fusion rules), but no such checks are supplied; the interpretive claim therefore does not follow from the overlap identity alone.
Simulated Author's Rebuttal
We thank the referee for the careful reading and the constructive comments on the abstract. We agree that the presentation of the central claim and the strength of the analogy can be improved for clarity and verifiability. We address each major comment below and will incorporate revisions in the next version of the manuscript.
read point-by-point responses
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Referee: [Abstract] Abstract: the central claim that a moment of the DSSYK transfer matrix equals the ASEP overlap is asserted without derivation, intermediate steps, explicit equations, or verification against the models' definitions, so the equality cannot be checked from the manuscript's content.
Authors: The derivation of the overlap identity is given in full in Sections 2–4 of the manuscript, beginning from the explicit definition of the DSSYK transfer matrix, the stationary distribution of ASEP, and the combinatorial evaluation of the moments that yields the product-state overlap. We nevertheless accept that the abstract is overly concise and does not contain the intermediate expressions needed for immediate verification. We will revise the abstract to include the key defining equations and a pointer to the relevant sections. revision: yes
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Referee: [Abstract] Abstract (final sentence): the argument that the identified overlap functions as the direct analogue of the strange correlator requires explicit verification that it reproduces key properties (invariance under local moves, relation to a topological invariant, or matching under anyon fusion rules), but no such checks are supplied; the interpretive claim therefore does not follow from the overlap identity alone.
Authors: The manuscript presents the analogy on the basis of the structural identity between the ASEP overlap and the definition of the strange correlator in the Levin–Wen/Turaev–Viro setting. We agree, however, that explicit checks of invariance properties and topological invariance would strengthen the claim. We will add a dedicated subsection that verifies these properties for the overlap in question. revision: yes
Circularity Check
No circularity; derivation is an explicit mapping plus interpretive analogy.
full rationale
The paper's core step is an explicit identity equating a DSSYK transfer-matrix moment to an ASEP stationary-state overlap with a product state. This identity is presented as a derived result rather than a definition or a fit renamed as a prediction. The subsequent claim that the overlap functions as an analogue of the strange correlator is an interpretive argument, not a reduction of the result to its own inputs by construction. No self-citations, ansatzes smuggled via prior work, or uniqueness theorems are invoked in a load-bearing way within the given abstract and description. The mapping can be checked independently of the analogy, so the derivation chain does not collapse.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
Black Holes and Random Matrices,
J. S. Cotler, G. Gur-Ari, M. Hanada, J. Polchinski, P. Saad, S. H. Shenker, D. Stanford, A. Streicher, and M. Tezuka, “Black Holes and Random Matrices,” JHEP05(2017) 118, arXiv:1611.04650 [hep-th]. [Erratum: JHEP 09, 002 (2018)]
Pith/arXiv arXiv 2017
-
[2]
Towards a full solution of the large N double-scaled SYK model,
M. Berkooz, M. Isachenkov, V. Narovlansky, and G. Torrents, “Towards a full solution of the large N double-scaled SYK model,” JHEP03(2019) 079,arXiv:1811.02584 [hep-th]
Pith/arXiv arXiv 2019
-
[3]
Correlators of double scaled SYK at one-loop,
K. Okuyama and K. Suzuki, “Correlators of double scaled SYK at one-loop,” JHEP05 (2023) 117,arXiv:2303.07552 [hep-th]
arXiv 2023
-
[4]
End of the world brane in double scaled SYK,
K. Okuyama, “End of the world brane in double scaled SYK,” JHEP08(2023) 053, arXiv:2305.12674 [hep-th]
arXiv 2023
-
[5]
Holographic tensor network for double-scaled SYK,
K. Okuyama, “Holographic tensor network for double-scaled SYK,” SciPost Phys.19no. 4, (2025) 083,arXiv:2503.23003 [hep-th]
arXiv 2025
-
[6]
M. Watanabe, “A JT/KPZ correspondence,”arXiv:2511.02529 [hep-th]. – 11 –
-
[7]
Exact solution of a 1d asymmetric exclusion model using a matrix formulation,
B. Derrida, M. R. Evans, V. Hakim, and V. Pasquier, “Exact solution of a 1d asymmetric exclusion model using a matrix formulation,” Journal of Physics A: Mathematical and General26no. 7, (1993) 1493–1517
1993
-
[8]
Exact solution of a partially asymmetric exclusion model using a deformed oscillator algebra,
R. A. Blythe, M. R. Evans, F. Colaiori, and F. H. Essler, “Exact solution of a partially asymmetric exclusion model using a deformed oscillator algebra,” Journal of Physics A: Mathematical and General33no. 12, (2000) 2313,arXiv:cond-mat/9910242 [cond-mat]
Pith/arXiv arXiv 2000
-
[9]
Integrable approach to simple exclusion processes with boundaries. Review and progress,
N. Crampe, E. Ragoucy, and M. Vanicat, “Integrable approach to simple exclusion processes with boundaries. Review and progress,” J. Stat. Mech.1411no. 11, (2014) P11032, arXiv:1408.5357 [math-ph]
Pith/arXiv arXiv 2014
-
[10]
String net condensation: A Physical mechanism for topological phases,
M. A. Levin and X.-G. Wen, “String net condensation: A Physical mechanism for topological phases,” Phys. Rev. B71(2005) 045110,arXiv:cond-mat/0404617
Pith/arXiv arXiv 2005
-
[11]
Wave function and strange correlator of short-range entangled states
Y.-Z. You, Z. Bi, A. Rasmussen, K. Slagle, and C. Xu, “Wave function and strange correlator of short-range entangled states.” Phys. Rev. Lett.112 24(2013) 247202,arXiv:1312.0626 [cond-mat.str-el]
Pith/arXiv arXiv 2013
-
[12]
Mapping topological to conformal field theories through strange correlators,
R. Vanhove, M. Bal, D. J. Williamson, N. Bultinck, J. Haegeman, and F. Verstraete, “Mapping topological to conformal field theories through strange correlators,” Phys. Rev. Lett.121no. 17, (2018) 177203,arXiv:1801.05959 [quant-ph]
Pith/arXiv arXiv 2018
-
[13]
Microscopic description of 2d topological phases, duality and 3d state sums,
Z. Kadar, A. Marzuoli, and M. Rasetti, “Microscopic description of 2d topological phases, duality and 3d state sums,” Adv. Math. Phys.2010(2010) 671039,arXiv:0907.3724 [quant-ph]
Pith/arXiv arXiv 2010
-
[14]
Quantum computation with Turaev–Viro codes,
R. Koenig, G. Kuperberg, and B. W. Reichardt, “Quantum computation with Turaev–Viro codes,” Annals Phys.325no. 12, (2010) 2707–2749,arXiv:1002.2816 [quant-ph]
Pith/arXiv arXiv 2010
-
[15]
String-net model of Turaev-Viro invariants,
A. Kirillov Jr, “String-net model of Turaev-Viro invariants,”arXiv:1106.6033 [math.AT]
-
[16]
Topological holography, quantum criticality, and boundary states,
S.-J. Huang and M. Cheng, “Topological holography, quantum criticality, and boundary states,” SciPost Phys.18no. 6, (2025) 213,arXiv:2310.16878 [cond-mat.str-el]
arXiv 2025
-
[17]
Duality via sequential quantum circuit in the topological holography formalism,
R. Vanhove, V. Ravindran, D. T. Stephen, X.-G. Wen, and X. Chen, “Duality via sequential quantum circuit in the topological holography formalism,” Phys. Rev. B112no. 3, (2025) 035173,arXiv:2409.06647 [cond-mat.str-el]
arXiv 2025
-
[18]
Entropic order parameters and topological holography,
H.-C. Zhang, G. Sierra, and J. Molina-Vilaplana, “Entropic order parameters and topological holography,”arXiv:2512.24225 [hep-th]
-
[19]
Gapless spin-fluid ground state in a random quantum heisenberg magnet,
S. Sachdev and J. Ye, “Gapless spin-fluid ground state in a random quantum heisenberg magnet,” Phys. Rev. Lett.70no. 21, (1993) 3339–3342,arXiv:cond-mat/9212030
Pith/arXiv arXiv 1993
-
[20]
A simple model of quantum holography (part 1),
A. Kitaev, “A simple model of quantum holography (part 1),”. https://online.kitp.ucsb.edu/online/entangled15/kitaev/
-
[21]
A simple model of quantum holography (part 2),
A. Kitaev, “A simple model of quantum holography (part 2),”. https://online.kitp.ucsb.edu/online/entangled15/kitaev2/
-
[22]
Doubled Hilbert space in double-scaled SYK,
K. Okuyama, “Doubled Hilbert space in double-scaled SYK,” JHEP04(2024) 091, arXiv:2401.07403 [hep-th]
arXiv 2024
-
[23]
Topological Defects on the Lattice: Dualities and Degeneracies,
D. Aasen, P. Fendley, and R. S. K. Mong, “Topological Defects on the Lattice: Dualities and Degeneracies,”arXiv:2008.08598 [cond-mat.stat-mech]
arXiv 2008
-
[24]
Matrix product – 12 – operator symmetries and intertwiners in string-nets with domain walls,
L. Lootens, J. Fuchs, J. Haegeman, C. Schweigert, and F. Verstraete, “Matrix product – 12 – operator symmetries and intertwiners in string-nets with domain walls,” SciPost Phys.10 no. 3, (2021) 053,arXiv:2008.11187 [quant-ph]
arXiv 2021
-
[25]
State sum invariants of 3-manifolds and quantum 6j-symbols,
V. G. Turaev and O. Y. Viro, “State sum invariants of 3-manifolds and quantum 6j-symbols,” Topology31no. 4, (1992) 865–902
1992
-
[26]
Invariants of piecewise linear three manifolds,
J. W. Barrett and B. W. Westbury, “Invariants of piecewise linear three manifolds,” Trans. Am. Math. Soc.348(1996) 3997–4022,arXiv:hep-th/9311155
Pith/arXiv arXiv 1996
-
[27]
Tensor-product representations for string-net condensed states,
Z.-C. Gu, M. Levin, B. Swingle, and X.-G. Wen, “Tensor-product representations for string-net condensed states,” Phys. Rev. B79no. 8, (2009) 085118,arXiv:0809.2821 [cond-mat.str-el]
Pith/arXiv arXiv 2009
-
[28]
Explicit tensor network representation for the ground states of string-net models,
O. Buerschaper, M. Aguado, and G. Vidal, “Explicit tensor network representation for the ground states of string-net models,” Phys. Rev. B79no. 8, (2009) 085119, arXiv:0809.2393 [cond-mat.str-el]
Pith/arXiv arXiv 2009
-
[29]
Fault tolerant quantum computation by anyons,
A. Y. Kitaev, “Fault tolerant quantum computation by anyons,” Annals Phys.303(2003) 2–30,arXiv:quant-ph/9707021
Pith/arXiv arXiv 2003
-
[30]
Quantum circuits for measuring Levin-Wen operators,
N. E. Bonesteel and D. P. DiVincenzo, “Quantum circuits for measuring Levin-Wen operators,” Phys. Rev. B86no. 16, (2012) 165113,arXiv:1206.6048 [quant-ph]
Pith/arXiv arXiv 2012
-
[31]
Quantum Error Correction Thresholds for the Universal Fibonacci Turaev-Viro Code,
A. Schotte, G. Zhu, L. Burgelman, and F. Verstraete, “Quantum Error Correction Thresholds for the Universal Fibonacci Turaev-Viro Code,” Phys. Rev. X12no. 2, (2022) 021012,arXiv:2012.04610 [quant-ph]
arXiv 2022
-
[32]
Bulk Locality and Quantum Error Correction in AdS/CFT,
A. Almheiri, X. Dong, and D. Harlow, “Bulk Locality and Quantum Error Correction in AdS/CFT,” JHEP04(2015) 163,arXiv:1411.7041 [hep-th]
Pith/arXiv arXiv 2015
-
[33]
Holographic quantum error-correcting codes: Toy models for the bulk/boundary correspondence,
F. Pastawski, B. Yoshida, D. Harlow, and J. Preskill, “Holographic quantum error-correcting codes: Toy models for the bulk/boundary correspondence,” JHEP06(2015) 149, arXiv:1503.06237 [hep-th]
Pith/arXiv arXiv 2015
-
[34]
Conformal symmetry and its breaking in two dimensional Nearly Anti-de-Sitter space,
J. Maldacena, D. Stanford, and Z. Yang, “Conformal symmetry and its breaking in two dimensional Nearly Anti-de-Sitter space,” PTEP2016no. 12, (2016) 12C104, arXiv:1606.01857 [hep-th]
Pith/arXiv arXiv 2016
-
[35]
JT gravity as a matrix integral,
P. Saad, S. H. Shenker, and D. Stanford, “JT gravity as a matrix integral,” arXiv:1903.11115 [hep-th]
Pith/arXiv arXiv 1903
-
[36]
The dilaton gravity hologram of double-scaled SYK,
A. Blommaert, T. G. Mertens, and J. Papalini, “The dilaton gravity hologram of double-scaled SYK,”arXiv:2404.03535 [hep-th]
-
[37]
An entropic puzzle in periodic dilaton gravity and DSSYK,
A. Blommaert, A. Levine, T. G. Mertens, J. Papalini, and K. Parmentier, “An entropic puzzle in periodic dilaton gravity and DSSYK,”arXiv:2411.16922 [hep-th]
-
[38]
Eight vertex SOS model and generalized Rogers-Ramanujan type identities,
G. E. Andrews, R. J. Baxter, and P. J. Forrester, “Eight vertex SOS model and generalized Rogers-Ramanujan type identities,” J. Statist. Phys.35(1984) 193–266
1984
-
[39]
Topological Defects on the Lattice I: The Ising model,
D. Aasen, R. S. K. Mong, and P. Fendley, “Topological Defects on the Lattice I: The Ising model,” J. Phys. A49no. 35, (2016) 354001,arXiv:1601.07185 [cond-mat.stat-mech]
Pith/arXiv arXiv 2016
-
[40]
The bulk Hilbert space of double scaled SYK,
H. W. Lin, “The bulk Hilbert space of double scaled SYK,” JHEP11(2022) 060, arXiv:2208.07032 [hep-th]
arXiv 2022
-
[41]
Kitaev’s Lattice Model and Turaev-Viro TQFTs,
B. Balsam and A. Kirillov Jr, “Kitaev’s Lattice Model and Turaev-Viro TQFTs,” arXiv:1206.2308 [math.QA]. – 13 –
-
[42]
D. L. Jafferis, D. K. Kolchmeyer, B. Mukhametzhanov, and J. Sonner, “Jackiw-Teitelboim gravity with matter, generalized eigenstate thermalization hypothesis, and random matrices,” Phys. Rev. D108no. 6, (2023) 066015,arXiv:2209.02131 [hep-th]
arXiv 2023
-
[43]
Integrable structure of conformal field theory II. Q operator and DDV equation,
V. V. Bazhanov, S. L. Lukyanov, and A. B. Zamolodchikov, “Integrable structure of conformal field theory II. Q operator and DDV equation,” Commun. Math. Phys.190 (1997) 247–278,arXiv:hep-th/9604044
Pith/arXiv arXiv 1997
-
[44]
Integrable structure of conformal field theory III. The Yang-Baxter relation,
V. V. Bazhanov, S. L. Lukyanov, and A. B. Zamolodchikov, “Integrable structure of conformal field theory III. The Yang-Baxter relation,” Commun. Math. Phys.200(1999) 297–324,arXiv:hep-th/9805008
Pith/arXiv arXiv 1999
-
[45]
An Ising-type formulation of the six-vertex model,
V. V. Bazhanov and S. M. Sergeev, “An Ising-type formulation of the six-vertex model,” Nucl. Phys. B986(2023) 116055,arXiv:2205.10708 [math-ph]
arXiv 2023
-
[46]
Shadow links and face models of statistical mechanics,
V. G. Turaev, “Shadow links and face models of statistical mechanics,” Journal of Differential Geometry36no. 1, (1992) 35–74
1992
-
[47]
Space-time random tensor networks and holographic duality,
X.-L. Qi and Z. Yang, “Space-time random tensor networks and holographic duality,” arXiv:1801.05289 [hep-th]
-
[48]
Solving 3d gravity with Virasoro TQFT,
S. Collier, L. Eberhardt, and M. Zhang, “Solving 3d gravity with Virasoro TQFT,” SciPost Phys.15no. 4, (2023) 151,arXiv:2304.13650 [hep-th]
arXiv 2023
-
[49]
3d gravity from Virasoro TQFT: Holography, wormholes and knots,
S. Collier, L. Eberhardt, and M. Zhang, “3d gravity from Virasoro TQFT: Holography, wormholes and knots,” SciPost Phys.17(2024) 134,arXiv:2401.13900 [hep-th]
arXiv 2024
-
[50]
T. Hartman, “Conformal Turaev-Viro Theory,”arXiv:2507.11652 [hep-th]
-
[51]
Triangulating quantum gravity in AdS 3,
T. Hartman, “Triangulating quantum gravity in AdS 3,”arXiv:2507.12696 [hep-th]
-
[52]
Random statistics of OPE coefficients and Euclidean wormholes,
A. Belin and J. de Boer, “Random statistics of OPE coefficients and Euclidean wormholes,” Class. Quant. Grav.38no. 16, (2021) 164001,arXiv:2006.05499 [hep-th]
arXiv 2021
-
[53]
Semiclassical 3D gravity as an average of large-c CFTs,
J. Chandra, S. Collier, T. Hartman, and A. Maloney, “Semiclassical 3D gravity as an average of large-c CFTs,” JHEP12(2022) 069,arXiv:2203.06511 [hep-th]
arXiv 2022
-
[54]
Approximate CFTs and random tensor models,
A. Belin, J. de Boer, D. L. Jafferis, P. Nayak, and J. Sonner, “Approximate CFTs and random tensor models,” JHEP09(2024) 163,arXiv:2308.03829 [hep-th]
arXiv 2024
-
[55]
3d gravity as a random ensemble,
D. L. Jafferis, L. Rozenberg, and G. Wong, “3d gravity as a random ensemble,” JHEP02 (2025) 208,arXiv:2407.02649 [hep-th]
arXiv 2025
-
[56]
On random matrix statistics of 3d gravity,
D. L. Jafferis, L. Rozenberg, D. Sarkar, and D. Wang, “On random matrix statistics of 3d gravity,”arXiv:2512.05045 [hep-th]
-
[57]
TQFT gravity and ensemble holography,
A. Dymarsky and A. Shapere, “TQFT gravity and ensemble holography,” JHEP02(2025) 091,arXiv:2405.20366 [hep-th]
arXiv 2025
-
[58]
Puzzles in 3D off-shell geometries via VTQFT,
C. Yan, “Puzzles in 3D off-shell geometries via VTQFT,” JHEP09(2025) 104, arXiv:2502.16686 [hep-th]
arXiv 2025
-
[59]
Surgery and statistics in 3d gravity,
J. de Boer, J. Kames-King, and B. Post, “Surgery and statistics in 3d gravity,” arXiv:2506.04151 [hep-th]
- [60]
-
[61]
A solvable model of 3d quantum gravity,
A. Dymarsky, “A solvable model of 3d quantum gravity,”arXiv:2605.12590 [hep-th]
-
[62]
A universal sum over topologies in 3d gravity,
A. Belin, S. Collier, L. Eberhardt, D. Liska, and B. Post, “A universal sum over topologies in 3d gravity,”arXiv:2601.07906 [hep-th]. – 14 –
-
[63]
QG from SymQRG: AdS 3/CFT2 Correspondence as Topological Symmetry-Preserving Quantum RG Flow,
N. Bao, L.-Y. Hung, Y. Jiang, and Z. Liu, “QG from SymQRG: AdS 3/CFT2 Correspondence as Topological Symmetry-Preserving Quantum RG Flow,”arXiv:2412.12045 [hep-th]. – 15 –
discussion (0)
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