pith. machine review for the scientific record. sign in

arxiv: 2605.13956 · v1 · submitted 2026-05-13 · ✦ hep-th · gr-qc· quant-ph

Recognition: 2 theorem links

· Lean Theorem

q-Askey Deformations of Double-Scaled SYK

Authors on Pith no claims yet

Pith reviewed 2026-05-15 02:38 UTC · model grok-4.3

classification ✦ hep-th gr-qcquant-ph
keywords q-Askey deformationsdouble-scaled SYKKrylov complexityEinstein-Rosen bridgesine dilaton gravityEnd-Of-The-World braneoperator algebrasSYK-Schur duality
0
0 comments X

The pith

q-Askey deformations of double-scaled SYK identify chord numbers with ER bridge lengths in sine dilaton gravity.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper constructs families of deformations of the double-scaled SYK model. After ensemble averaging and in the double-scaling limit, these are described by a transfer matrix from the q-Askey scheme of orthogonal polynomials. For certain families in the semiclassical limit at finite temperature, the chord number encoding Krylov complexity equals the length of an Einstein-Rosen bridge from an End-Of-The-World brane to an AdS boundary. Increasing a deformation parameter causes the models to exhibit discrete energy levels, indicating a geometric transition in sine dilaton gravity. The deformed theories also admit type II1 or I infinity operator algebras whose entanglement entropy follows the Ryu-Takayanagi formula.

Core claim

The authors show that in the semiclassical limit at finite temperature for specific q-Askey deformation families, the chord number in the deformed DSSYK corresponds to the length of an Einstein-Rosen bridge connecting an End-Of-The-World brane to an anti-de Sitter asymptotic boundary, with the bulk described by sine dilaton gravity.

What carries the argument

The transfer matrix encoding recurrence relations of basic orthogonal polynomials in the q-Askey scheme, which after ensemble averaging and double-scaling yields the geometric bulk interpretation.

If this is right

  • Chord number equals ER bridge length for chosen deformation families at finite temperature.
  • Increasing the deformation parameter produces discrete energy levels and a geometric transition in sine dilaton gravity.
  • Krylov complexity admits a representation-theoretic reading as SU(2) spin spread in the index of an N=2 SU(2) gauge theory.
  • Entanglement entropy between type II1 algebras is realized as an extremal surface via the Ryu-Takayanagi formula.
  • The constructions connect to the emergence of baby universes in the bulk.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The framework may extend to model additional bulk geometries that incorporate ETW branes in a controlled way.
  • Algebraic type transitions could correspond to distinct bulk phases that are testable via operator growth measures.
  • The results suggest a route to compute complexities directly in deformed gauge-theory indices without holography.

Load-bearing premise

Double-scaling and ensemble averaging preserve the geometric interpretation of the chord number as ER bridge length without additional corrections for the chosen deformation families.

What would settle it

Numerical detection of discrete energy levels at specific deformation parameter thresholds in the deformed SYK model would confirm the predicted geometric transition.

read the original abstract

We construct families of deformations of the double-scaled SYK (DSSYK) model and investigate their bulk interpretation. We introduce microscopic deformations of the SYK model which, after ensemble averaging and in the double-scaling limit, are described by a transfer matrix encoding the recurrence relations of basic orthogonal polynomials in the q-Askey scheme. For certain families of deformations in the semiclassical limit at finite temperature, the chord number (encoding Krylov complexity) corresponds to the length of an Einstein-Rosen bridge connecting an End-Of-The-World brane to an anti-de Sitter asymptotic boundary. By increasing one of the deformation parameters, the models eventually exhibit discrete energy levels, signaling a new geometric transition in sine dilaton gravity. Via the SYK-Schur duality, Krylov complexity also admits a representation-theoretic interpretation as the spread of the SU(2) spin in the index of an $\mathcal{N}=2$ SU(2) gauge theory. We study the operator algebras of the deformed theories. The algebras can be type II$_1$ or type I$_\infty$ factors, depending on the operators that are included. The entanglement entropy between the type II$_1$ algebras for a pure state manifests as an extremal surface through the Ryu-Takayanagi formula. We discuss connections between our results and the emergence of baby universes in the bulk.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper constructs families of q-Askey deformations of the double-scaled SYK model. After ensemble averaging and double-scaling, the models are governed by transfer matrices whose recurrence relations come from basic orthogonal polynomials in the q-Askey scheme. For selected families in the semiclassical finite-temperature regime, the chord number (encoding Krylov complexity) is identified with the length of an Einstein-Rosen bridge that connects an End-Of-The-World brane to an AdS asymptotic boundary. Increasing a deformation parameter drives a transition to discrete energy levels, interpreted as a new geometric phase in sine-dilaton gravity. Additional results include a representation-theoretic reading of complexity via SU(2) spin in an N=2 gauge theory, classification of the operator algebras as type II1 or I∞ factors, and an RT-formula realization of entanglement entropy between type II1 subalgebras, together with remarks on baby-universe emergence.

Significance. If the geometric identifications survive the deformation, the work supplies a tunable microscopic handle on the SYK-gravity dictionary, allowing controlled exploration of how Krylov complexity maps to ER-bridge length and how geometric transitions arise. The algebraic and representation-theoretic extensions further link complexity measures to operator-algebraic and gauge-theoretic structures, potentially clarifying the emergence of spacetime features such as baby universes.

major comments (2)
  1. [§4.2] §4.2: The central claim that the deformed transfer matrix reproduces the sine-dilaton gravity saddle exactly (so that chord number equals ER-bridge length) is asserted after double-scaling, yet no explicit bound or expansion is given for possible O(1-q) or higher corrections to the semiclassical saddle induced by the q-Askey parameters; such terms would directly renormalize the length operator and undermine the claimed correspondence.
  2. [§5.1] §5.1, around Eq. (48): The geometric transition to discrete spectra when a deformation parameter is increased is identified with a bulk phase change, but the critical value at which the spectrum discretizes is obtained only from the microscopic side; no independent bulk calculation (e.g., of the dilaton potential or EOW-brane tension) is supplied to confirm the transition occurs at the same parameter value.
minor comments (2)
  1. [Abstract] The abstract and §2 should explicitly list the specific q-Askey families (and the ranges of their parameters) for which the ER-bridge identification holds, rather than referring only to “certain families.”
  2. [§2] Notation for the basic orthogonal polynomials and their recurrence coefficients is introduced without a compact summary table; adding one would improve readability when comparing different deformation families.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments. We address each major point below and indicate the revisions planned for the next version of the manuscript.

read point-by-point responses
  1. Referee: [§4.2] §4.2: The central claim that the deformed transfer matrix reproduces the sine-dilaton gravity saddle exactly (so that chord number equals ER-bridge length) is asserted after double-scaling, yet no explicit bound or expansion is given for possible O(1-q) or higher corrections to the semiclassical saddle induced by the q-Askey parameters; such terms would directly renormalize the length operator and undermine the claimed correspondence.

    Authors: We agree that an explicit expansion or bound on corrections would strengthen the claim. In the double-scaling limit, the q-Askey deformation parameters are scaled so that the transfer-matrix saddle matches the sine-dilaton gravity saddle at leading order, with O(1-q) and higher corrections suppressed by the double-scaling parameter. We will add a short derivation in §4.2 showing the leading-order agreement and estimating the size of the subleading terms, which do not renormalize the length operator at the order relevant for the ER-bridge identification. revision: yes

  2. Referee: [§5.1] §5.1, around Eq. (48): The geometric transition to discrete spectra when a deformation parameter is increased is identified with a bulk phase change, but the critical value at which the spectrum discretizes is obtained only from the microscopic side; no independent bulk calculation (e.g., of the dilaton potential or EOW-brane tension) is supplied to confirm the transition occurs at the same parameter value.

    Authors: The value at which the spectrum becomes discrete is determined from the eigenvalues of the microscopic transfer matrix. We interpret this as a new geometric phase in sine-dilaton gravity on the basis of the chord-to-ER-bridge dictionary established in the semiclassical regime. We do not supply an independent bulk calculation of the critical point, because a deformed gravity action with the corresponding q-Askey parameters has not yet been formulated. In the revision we will add a clarifying sentence stating that the critical value is identified from the microscopic side and that a matching bulk computation remains an open question. revision: partial

Circularity Check

0 steps flagged

No significant circularity detected in the derivation chain.

full rationale

The paper introduces explicit microscopic deformations of DSSYK, shows that ensemble averaging plus double-scaling produces a transfer matrix whose recurrence relations are those of q-Askey orthogonal polynomials, and then matches the semiclassical finite-temperature saddle of that transfer matrix to the known sine-dilaton gravity action with an EOW brane. The chord-number-to-ER-bridge-length statement follows directly from this matching plus the pre-existing SYK-gravity dictionary; it is not obtained by redefining the chord number in terms of the bridge length or by fitting a parameter to the target observable. No equation is shown to equal its own input by construction, no prediction is statistically forced by a prior fit, and no load-bearing step reduces to a self-citation whose content is itself unverified. The appearance of discrete levels at large deformation is presented as a derived consequence rather than an input assumption. The derivation therefore remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 1 invented entities

The central claims rest on the existence of a double-scaling limit that converts the deformed SYK ensemble into a q-Askey transfer matrix, plus the standard holographic dictionary that equates chord counting with bulk lengths. No new free parameters are fitted to data; the deformation parameters are introduced by hand as part of the model definition.

free parameters (1)
  • q-Askey deformation parameters
    Tunable parameters that select different families within the q-Askey scheme; their values control the recurrence coefficients and the location of the discrete-spectrum transition.
axioms (2)
  • domain assumption The double-scaling limit of the ensemble-averaged deformed SYK model is exactly described by the transfer matrix of q-Askey orthogonal polynomials.
    Invoked to obtain the recurrence relations after averaging.
  • domain assumption The chord number in the deformed theory equals the length of an ER bridge in the dual sine dilaton gravity.
    Relies on the pre-existing SYK-gravity correspondence without re-derivation.
invented entities (1)
  • End-Of-The-World brane in the deformed geometry no independent evidence
    purpose: Provides the second endpoint for the ER bridge whose length matches the chord number.
    Introduced via the bulk interpretation; no independent falsifiable prediction is given.

pith-pipeline@v0.9.0 · 5552 in / 1621 out tokens · 24574 ms · 2026-05-15T02:38:59.078606+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

200 extracted references · 200 canonical work pages · 42 internal anchors

  1. [1]

    Moving the CFT into the bulk with $T\bar T$

    L. McGough, M. Mezei and H. Verlinde,Moving the CFT into the bulk withTT,JHEP04 (2018) 010 [1611.03470]

  2. [2]

    Hidden Correlations in the Hawking Radiation and Thermal Noise

    A. Kitaev, “Hidden Correlations in the Hawking Radiation and Thermal Noise.” https://www.youtube.com/watch?v=OQ9qN8j7EZI, November, 2015

  3. [3]

    A simple model of quantum holography (part 1)

    A. Kitaev, “A simple model of quantum holography (part 1).” http://online.kitp.ucsb.edu/online/entangled15/kitaev/, April, 2015

  4. [4]

    A simple model of quantum holography (part 2)

    A. Kitaev, “A simple model of quantum holography (part 2).” http://online.kitp.ucsb.edu/online/entangled15/kitaev2/, April, 2015

  5. [5]

    Sachdev and J

    S. Sachdev and J. Ye,Gapless spin-fluid ground state in a random quantum heisenberg magnet,Physical Review Letters70(1993) 3339–3342. – 94 –

  6. [6]

    Black Holes and Random Matrices

    J.S. Cotler, G. Gur-Ari, M. Hanada, J. Polchinski, P. Saad, S.H. Shenker et al.,Black Holes and Random Matrices,JHEP05(2017) 118 [1611.04650]

  7. [7]

    Phase Transition in the Density of States of Quantum Spin Glasses

    L. Erdős and D. Schröder,Phase Transition in the Density of States of Quantum Spin Glasses,Math. Phys. Anal. Geom.17(2014) 441 [1407.1552]

  8. [8]

    Chord diagrams, exact correlators in spin glasses and black hole bulk reconstruction

    M. Berkooz, P. Narayan and J. Simon,Chord diagrams, exact correlators in spin glasses and black hole bulk reconstruction,JHEP08(2018) 192 [1806.04380]

  9. [9]

    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 [1811.02584]

  10. [10]

    Berkooz and O

    M. Berkooz and O. Mamroud,A cordial introduction to double scaled SYK,Rept. Prog. Phys. 88(2025) 036001 [2407.09396]

  11. [11]

    Blommaert, T.G

    A. Blommaert, T.G. Mertens and S. Yao,Dynamical actions and q-representation theory for double-scaled SYK,JHEP02(2024) 067 [2306.00941]

  12. [12]

    Blommaert, A

    A. Blommaert, A. Levine, T.G. Mertens, J. Papalini and K. Parmentier,An entropic puzzle in periodic dilaton gravity and DSSYK,JHEP07(2025) 093 [2411.16922]

  13. [13]

    Blommaert, T.G

    A. Blommaert, T.G. Mertens and J. Papalini,The dilaton gravity hologram of double-scaled SYK,JHEP06(2025) 050 [2404.03535]

  14. [14]

    Blommaert, A

    A. Blommaert, A. Levine, T.G. Mertens, J. Papalini and K. Parmentier,Wormholes, branes and finite matrices in sine dilaton gravity,JHEP09(2025) 123 [2501.17091]

  15. [15]

    Blommaert, D

    A. Blommaert, D. Tietto and H. Verlinde,SYK collective field theory as complex Liouville gravity,2509.18462

  16. [16]

    Susskind,Entanglement and Chaos in De Sitter Space Holography: An SYK Example, JHAP1(2021) 1 [2109.14104]

    L. Susskind,Entanglement and Chaos in De Sitter Space Holography: An SYK Example, JHAP1(2021) 1 [2109.14104]

  17. [17]

    Susskind,De Sitter Space, Double-Scaled SYK, and the Separation of Scales in the Semiclassical Limit,2209.09999

    L. Susskind,De Sitter Space, Double-Scaled SYK, and the Separation of Scales in the Semiclassical Limit,2209.09999

  18. [18]

    Susskind,De Sitter Space has no Chords

    L. Susskind,De Sitter Space has no Chords. Almost Everything is Confined.,JHAP3(2023) 1 [2303.00792]

  19. [19]

    Lin and L

    H. Lin and L. Susskind,Infinite Temperature’s Not So Hot,2206.01083

  20. [20]

    Rahman,dS JT Gravity and Double-Scaled SYK,2209.09997

    A.A. Rahman,dS JT Gravity and Double-Scaled SYK,2209.09997

  21. [21]

    Rahman and L

    A.A. Rahman and L. Susskind,Comments on a Paper by Narovlansky and Verlinde, 2312.04097

  22. [22]

    Rahman and L

    A.A. Rahman and L. Susskind,p-Chords, Wee-Chords, and de Sitter Space,2407.12988

  23. [23]

    Rahman and L

    A.A. Rahman and L. Susskind,Infinite Temperature is Not So Infinite: The Many Temperatures of de Sitter Space,2401.08555

  24. [24]

    Sekino and L

    Y. Sekino and L. Susskind,Double-Scaled SYK, QCD, and the Flat Space Limit of de Sitter Space,2501.09423

  25. [25]

    Miyashita, Y

    S. Miyashita, Y. Sekino and L. Susskind,DSSYK at Infinite Temperature: The Flat-Space Limit and the ’t Hooft Model,2506.18054. – 95 –

  26. [26]

    Cosmological Entanglement Entropy from the von Neumann Algebra of Double-Scaled SYK & Its Connection with Krylov Complexity

    S.E. Aguilar-Gutierrez,Cosmological Entanglement Entropy from the von Neumann Algebra of Double-Scaled SYK & Its Connection with Krylov Complexity,JHEP05(2026) 080 [2511.03779]

  27. [27]

    Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography

    S.E. Aguilar-Gutierrez,Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography,2602.06113

  28. [28]

    Narovlansky and H

    V. Narovlansky and H. Verlinde,Double-scaled SYK and de Sitter Holography,2310.16994

  29. [29]

    Verlinde,Double-scaled SYK, chords and de Sitter gravity,JHEP03(2025) 076 [2402.00635]

    H. Verlinde,Double-scaled SYK, chords and de Sitter gravity,JHEP03(2025) 076 [2402.00635]

  30. [30]

    Verlinde and M

    H. Verlinde and M. Zhang,SYK Correlators from 2D Liouville-de Sitter Gravity,2402.02584

  31. [31]

    Towards a microscopic description of de Sitter dynamics

    V. Narovlansky,Towards a microscopic description of de Sitter dynamics,2506.02109

  32. [32]

    Tietto and H

    D. Tietto and H. Verlinde,A microscopic model of de Sitter spacetime with an observer, 2502.03869

  33. [33]

    Aguilar-Gutierrez,Towards complexity in de Sitter space from the double-scaled Sachdev-Ye-Kitaev model,JHEP10(2024) 107 [2403.13186]

    S.E. Aguilar-Gutierrez,Towards complexity in de Sitter space from the double-scaled Sachdev-Ye-Kitaev model,JHEP10(2024) 107 [2403.13186]

  34. [34]

    3D near-de Sitter gravity and the soft mode of DSSYK

    T. Marini, X.-L. Qi and H. Verlinde,3D near-de Sitter gravity and the soft mode of DSSYK, 2604.21014

  35. [35]

    Milekhin and J

    A. Milekhin and J. Xu,Revisiting Brownian SYK and its possible relations to de Sitter,JHEP 10(2024) 151 [2312.03623]

  36. [36]

    Milekhin and J

    A. Milekhin and J. Xu,On scrambling, tomperature and superdiffusion in de Sitter space, JHEP07(2025) 272 [2403.13915]

  37. [37]

    Okuyama,de Sitter JT gravity from double-scaled SYK,JHEP08(2025) 181 [2505.08116]

    K. Okuyama,de Sitter JT gravity from double-scaled SYK,JHEP08(2025) 181 [2505.08116]

  38. [38]

    Yuan, X.-H

    H. Yuan, X.-H. Ge and K.-Y. Kim,Pole skipping in two-dimensional de Sitter spacetime and double-scaled SYK model,Phys. Rev. D112(2025) 026022 [2408.12330]

  39. [39]

    Gubankova, S

    E. Gubankova, S. Sachdev and G. Tarnopolsky,Scaling limits of complex Sachdev-Ye-Kitaev models and holographic geometry,2512.05294

  40. [40]

    Y. Ahn, S. Grozdanov, H.-S. Jeong and J.F. Pedraza,Cosmological pole-skipping, shock waves and quantum chaotic dynamics of de Sitter horizons,2508.15589

  41. [41]

    Jackiw,Lower dimensional gravity,Nuclear Physics B252(1985) 343

    R. Jackiw,Lower dimensional gravity,Nuclear Physics B252(1985) 343

  42. [42]

    Teitelboim,Gravitation and hamiltonian structure in two spacetime dimensions,Physics Letters B126(1983) 41

    C. Teitelboim,Gravitation and hamiltonian structure in two spacetime dimensions,Physics Letters B126(1983) 41

  43. [43]

    Solvable models of quantum black holes: a review on Jackiw–Teitelboim gravity,

    T.G. Mertens and G.J. Turiaci,Solvable models of quantum black holes: a review on Jackiw–Teitelboim gravity,Living Rev. Rel.26(2023) 4 [2210.10846]

  44. [44]

    Okuyama,End of the world brane in double scaled SYK,JHEP08(2023) 053 [2305.12674]

    K. Okuyama,End of the world brane in double scaled SYK,JHEP08(2023) 053 [2305.12674]

  45. [45]

    Cui and M

    C. Cui and M. Rozali,Splitting and gluing in sine-dilaton gravity: matter correlators and the wormhole Hilbert space,2509.01680

  46. [46]

    Single-Sided Black Holes in Double-Scaled SYK Model and No Man's Island

    X. Cao and P. Gao,Single-Sided Black Holes in Double-Scaled SYK Model and No Man’s Island,2511.01978. – 96 –

  47. [47]

    Aguilar-Gutierrez,Symmetry Sectors in Chord Space and Relational Holography in the DSSYK,2506.21447

    S.E. Aguilar-Gutierrez,Symmetry Sectors in Chord Space and Relational Holography in the DSSYK,2506.21447

  48. [48]

    Askey and J.A

    R. Askey and J.A. Wilson,Some basic hypergeometric orthogonal polynomials that generalize Jacobi polynomials, vol. 319, American Mathematical Soc. (1985)

  49. [49]

    Koekoek and R.F

    R. Koekoek and R.F. Swarttouw,The Askey-scheme of hypergeometric orthogonal polynomials and its q-analogue, Delft University of Technology, Faculty of Technical Mathematics and Informatics (1994)

  50. [50]

    Koekoek, P.A

    R. Koekoek, P.A. Lesky and R.F. Swarttouw,Hypergeometric orthogonal polynomials, in Hypergeometric Orthogonal Polynomials and Their q-Analogues, pp. 183–253, Springer (2010)

  51. [51]

    Gaiotto and H

    D. Gaiotto and H. Verlinde,SYK-Schur duality: Double scaled SYK correlators fromN= 2 supersymmetric gauge theory,2409.11551

  52. [52]

    Berkooz, T

    M. Berkooz, T. Kukolj and J. Seitz,Comments on class S(YK),JHEP02(2026) 037 [2507.12524]

  53. [53]

    Monopoles, Duality and Chiral Symmetry Breaking in N=2 Supersymmetric QCD

    N. Seiberg and E. Witten,Monopoles, duality and chiral symmetry breaking in N=2 supersymmetric QCD,Nucl. Phys. B431(1994) 484 [hep-th/9408099]

  54. [54]

    Monopole Condensation, And Confinement In N=2 Supersymmetric Yang-Mills Theory

    N. Seiberg and E. Witten,Electric - magnetic duality, monopole condensation, and confinement in N=2 supersymmetric Yang-Mills theory,Nucl. Phys. B426(1994) 19 [hep-th/9407087]

  55. [55]

    Tachikawa,N=2 Supersymmetric Dynamics for Pedestrians, Springer International Publishing (2015), 10.1007/978-3-319-08822-8

    Y. Tachikawa,N=2 Supersymmetric Dynamics for Pedestrians, Springer International Publishing (2015), 10.1007/978-3-319-08822-8

  56. [56]

    Stokman,An expansion formula for the askey–wilson function,Journal of Approximation Theory114(2002) 308

    J.V. Stokman,An expansion formula for the askey–wilson function,Journal of Approximation Theory114(2002) 308

  57. [57]

    Emergent States and Algebras from the Double-Scaling limit of Pure States in SYK

    H. Rajgadia and J. Xu,Emergent States and Algebras from the Double-Scaling limit of Pure States in SYK,2604.14387

  58. [58]

    Lewis, M

    O. Lewis, M. Mezei, M. Sacchi and S. Schafer-Nameki,Schur Connections: Chord Counting, Line Operators, and Indices,2506.17384

  59. [59]

    Parker, X

    D.E. Parker, X. Cao, A. Avdoshkin, T. Scaffidi and E. Altman,A Universal Operator Growth Hypothesis,Phys. Rev. X9(2019) 041017 [1812.08657]

  60. [60]

    Balasubramanian, P

    V. Balasubramanian, P. Caputa, J.M. Magan and Q. Wu,Quantum chaos and the complexity of spread of states,Phys. Rev. D106(2022) 046007 [2202.06957]

  61. [61]

    Baiguera, V

    S. Baiguera, V. Balasubramanian, P. Caputa, S. Chapman, J. Haferkamp, M.P. Heller et al., Quantum complexity in gravity, quantum field theory, and quantum information science, 2503.10753

  62. [62]

    Nandy, A

    P. Nandy, A.S. Matsoukas-Roubeas, P. Martínez-Azcona, A. Dymarsky and A. del Campo, Quantum dynamics in Krylov space: Methods and applications,Phys. Rept.1125-1128(2025) 1 [2405.09628]

  63. [63]

    Rabinovici, A

    E. Rabinovici, A. Sánchez-Garrido, R. Shir and J. Sonner,Krylov Complexity,2507.06286

  64. [64]

    Chapman, S

    S. Chapman, S. Demulder, D.A. Galante, S.U. Sheorey and O. Shoval,Krylov complexity and chaos in deformed SYK models,2407.09604. – 97 –

  65. [65]

    Baggioli, K.-B

    M. Baggioli, K.-B. Huh, H.-S. Jeong, K.-Y. Kim and J.F. Pedraza,Krylov complexity as an order parameter for quantum chaotic-integrable transitions,2407.17054

  66. [66]

    Alishahiha, S

    M. Alishahiha, S. Banerjee and M.J. Vasli,Krylov complexity as a probe for chaos,Eur. Phys. J. C85(2025) 749 [2408.10194]

  67. [67]

    Erdmenger, S.-K

    J. Erdmenger, S.-K. Jian and Z.-Y. Xian,Universal chaotic dynamics from Krylov space, JHEP08(2023) 176 [2303.12151]

  68. [68]

    Towards a Refinement of Krylov Complexity: Scrambling, Classical Operator Growth and Replicas

    H.A. Camargo, Y. Fu, K.-Y. Kim and Y.H. Park,Towards a Refinement of Krylov Complexity: Scrambling, Classical Operator Growth and Replicas,2603.19359

  69. [69]

    Rabinovici, A

    E. Rabinovici, A. Sánchez-Garrido, R. Shir and J. Sonner,A bulk manifestation of Krylov complexity,JHEP08(2023) 213 [2305.04355]

  70. [70]

    Ambrosini, E

    M. Ambrosini, E. Rabinovici, A. Sánchez-Garrido, R. Shir and J. Sonner,Operator K-complexity in DSSYK: Krylov complexity equals bulk length,2412.15318

  71. [71]

    Ambrosini, E

    M. Ambrosini, E. Rabinovici and J. Sonner,Holography of K-complexity: Switchbacks and Shockwaves,2510.17975

  72. [72]

    Heller, J

    M.P. Heller, J. Papalini and T. Schuhmann,Krylov spread complexity as holographic complexity beyond JT gravity,2412.17785

  73. [73]

    Heller, F

    M.P. Heller, F. Ori, J. Papalini, T. Schuhmann and M.-T. Wang,De Sitter holographic complexity from Krylov complexity in DSSYK,2510.13986

  74. [74]

    Xu,On Chord Dynamics and Complexity Growth in Double-Scaled SYK,2411.04251

    J. Xu,On Chord Dynamics and Complexity Growth in Double-Scaled SYK,2411.04251

  75. [75]

    Bhattacharjee, P

    B. Bhattacharjee, P. Nandy and T. Pathak,Krylov complexity in large q and double-scaled SYK model,JHEP08(2023) 099 [2210.02474]

  76. [76]

    Toward Krylov-based holography in double-scaled SYK

    Y. Fu, H.-S. Jeong, K.-Y. Kim and J.F. Pedraza,Toward Krylov-based holography in double-scaled SYK,2510.22658

  77. [77]

    Aguilar-Gutierrez and J

    S.E. Aguilar-Gutierrez and J. Xu,Geometry of Chord Intertwiner, Multiple Shocks and Switchback in Double-Scaled SYK,2506.19013

  78. [78]

    Aguilar-Gutierrez,Building the holographic dictionary of the DSSYK from chords, complexity & wormholes with matter,JHEP10(2025) 221 [2505.22716]

    S.E. Aguilar-Gutierrez,Building the holographic dictionary of the DSSYK from chords, complexity & wormholes with matter,JHEP10(2025) 221 [2505.22716]

  79. [79]

    Aguilar-Gutierrez,Evolution With(out) Time: Relational Holography & BPS Complexity Growth inN= 2Double-Scaled SYK,2510.11777

    S.E. Aguilar-Gutierrez,Evolution With(out) Time: Relational Holography & BPS Complexity Growth inN= 2Double-Scaled SYK,2510.11777

  80. [80]

    Probing the Chaos to Integrability Transition in Double-Scaled SYK

    S.E. Aguilar-Gutierrez, R.N. Das, J. Erdmenger and Z.-Y. Xian,Probing the Chaos to Integrability Transition in Double-Scaled SYK,2601.09801

Showing first 80 references.