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arxiv: 2605.30007 · v1 · pith:RPJ7OYM5new · submitted 2026-05-28 · ❄️ cond-mat.stat-mech · hep-th· math-ph· math.MP· nlin.SI· quant-ph

Hidden Ising models from the generalized Yang-Baxter equation

Pith reviewed 2026-06-29 00:31 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech hep-thmath-phmath.MPnlin.SIquant-ph
keywords free-fermionic spectrumYang-Baxter equationIsing modelconserved quantitiesspin chainsmulti-site interactionsquantum inverse scattering
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The pith

A multi-site spin-1/2 chain has a free-fermionic spectrum with extra degeneracy from local conserved quantities that act like classical background fields.

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

The authors introduce a one-dimensional spin-1/2 Hamiltonian with local multi-site interactions. They observe that the algebra among its Hamiltonian density operators matches the algebra of the transverse-field Ising model. This match lets the spectrum be diagonalized in terms of free fermions, but each energy level acquires a large multiplicity from additional local conserved operators. Those operators behave as fixed classical fields superimposed on the quantum spins. The construction is obtained by adapting the quantum inverse scattering method to a multi-site version of the Yang-Baxter equation whose R-matrix is built from extraspecial 2-group generators.

Core claim

The introduced Hamiltonian has an algebra of densities that matches the transverse field Ising model, making its spectrum free-fermionic with huge degeneracy from local conserved quantities acting as classical background fields. It is obtained via the quantum inverse scattering method with a generalized Yang-Baxter equation using R-matrices from extraspecial 2-groups.

What carries the argument

The algebra of the Hamiltonian densities, which resembles that of the transverse-field Ising model and thereby permits a free-fermion mapping while preserving extra local charges.

If this is right

  • The thermodynamics differs from the ordinary Ising chain because of the extra degeneracy at each level.
  • At gapless points the model is recovered from the quantum inverse scattering method applied to the multi-site Yang-Baxter equation.
  • All conserved charges follow directly from the R-matrix built with extraspecial 2-group generators.
  • The same construction supplies a systematic way to produce other multi-site spin systems that are transverse-field Ising models underneath.
  • Fendley's free-fermion-in-disguise models can be recovered inside the same formalism.

Where Pith is reading between the lines

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

  • Numerical spectra of small chains should display a degeneracy pattern that factors into the Ising contribution times the dimension of the classical background configurations.
  • The extraspecial-group construction may extend to other root-of-unity or higher-rank cases, yielding families of hidden free-fermion models.
  • Physical realizations with engineered multi-spin couplings could exhibit unexpectedly flat bands or enhanced susceptibilities traceable to the hidden charges.
  • The method offers a route to classify integrable multi-site chains by the algebraic resemblance of their densities to known solvable models.

Load-bearing premise

The algebra satisfied by the Hamiltonian densities is assumed to be close enough to the transverse-field Ising model algebra that the spectrum remains free-fermionic.

What would settle it

Exact diagonalization of the Hamiltonian on chains of length 8-12, checking whether the eigenvalues follow the free-fermion dispersion and whether the observed multiplicities match the number of independent local conserved quantities.

Figures

Figures reproduced from arXiv: 2605.30007 by Akash Sinha, Pramod Padmanabhan, Somnath Maity, Vladimir Korepin.

Figure 1
Figure 1. Figure 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 1
Figure 1. Figure 1: FIG. 1: Action of the Hamiltonian density of (8). [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: A commutative diagram explaining various [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: (a) Periodic boundary conditions and (b) open boundary conditions. The energy eigenvalues of [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Thermodynamic properties of the hidden critical ( [PITH_FULL_IMAGE:figures/full_fig_p009_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Action of the Hamiltonian density of [PITH_FULL_IMAGE:figures/full_fig_p016_5.png] view at source ↗
read the original abstract

We introduce a one dimensional spin $\frac{1}{2}$ Hamiltonian with multi-site interactions, but still local. The algebra of its Hamiltonian densities resembles that of the transverse field Ising model. Using this fact we show that its spectrum is free-fermionic but with a huge degeneracy for each level. The source of the degeneracy is a set of local conserved quantities that act like a classical background field for the quantum system. The thermodynamics of this system is contrasted with the standard Ising model. At the gapless points in the energy spectrum, we show that this system can be derived from the quantum inverse scattering method adapted to a multi-site generalization of the Yang-Baxter equation as introduced by E. Rowell and Z. Wang. The $R$-matrix is constructed using generators of extraspecial 2-groups. This helps us extract all the conserved charges and lay the framework for a general mechanism to generate such multi-site interaction spin systems that are transverse field Ising models under the hood. A remark on how to obtain P. Fendley's free-fermion in disguise models in this formalism is also included.

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 / 1 minor

Summary. The manuscript introduces a one-dimensional spin-1/2 Hamiltonian with local multi-site interactions. It asserts that the algebra of the Hamiltonian densities resembles that of the transverse-field Ising model (TFIM), from which it concludes that the spectrum is free-fermionic with extensive degeneracy generated by a set of local conserved quantities that behave as a classical background field. The model is obtained from the quantum inverse scattering method applied to a multi-site generalization of the Yang-Baxter equation, with the R-matrix constructed from generators of extraspecial 2-groups; thermodynamics are contrasted with the ordinary Ising chain, and a remark on recovering Fendley-type models is included.

Significance. If the central algebraic claim is rigorously established, the construction supplies an explicit mechanism for generating families of integrable spin chains whose free-fermion character is hidden behind additional local integrals of motion. The link to the generalized Yang-Baxter equation and extraspecial 2-groups offers a potential route to systematic classification of such models beyond nearest-neighbor interactions.

major comments (2)
  1. [Abstract / Hamiltonian definition] Abstract and the paragraph following the definition of the Hamiltonian: the assertion that algebraic resemblance to the TFIM implies a free-fermionic spectrum is load-bearing for the central claim, yet the multi-site interaction terms are not shown to map under Jordan-Wigner to purely bilinear fermionic operators. An explicit verification that no quartic or higher fermionic terms survive is required; the TFIM case works because its nearest-neighbor terms become quadratic, but this does not automatically extend to the multi-site case without further proof.
  2. [Conserved quantities paragraph] Section on conserved quantities (the paragraph introducing the local charges that act as background fields): the degeneracy is attributed to these charges, but it is not demonstrated that they commute with the Hamiltonian while remaining independent of the fermionic degrees of freedom that diagonalize the quadratic part. An explicit commutation relation or counting argument establishing that the degeneracy is independent of system size and of the particular choice of R-matrix parameters would strengthen the claim.
minor comments (1)
  1. [Abstract] The abstract states that the R-matrix is constructed using generators of extraspecial 2-groups; a brief reminder of the defining relations of these groups (or a reference to the precise representation used) would aid readers unfamiliar with the construction.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We respond to each major point below, agreeing that additional explicit verifications will strengthen the presentation, and will incorporate them in the revised version.

read point-by-point responses
  1. Referee: [Abstract / Hamiltonian definition] Abstract and the paragraph following the definition of the Hamiltonian: the assertion that algebraic resemblance to the TFIM implies a free-fermionic spectrum is load-bearing for the central claim, yet the multi-site interaction terms are not shown to map under Jordan-Wigner to purely bilinear fermionic operators. An explicit verification that no quartic or higher fermionic terms survive is required; the TFIM case works because its nearest-neighbor terms become quadratic, but this does not automatically extend to the multi-site case without further proof.

    Authors: We agree that an explicit Jordan-Wigner transformation for the multi-site terms would clarify the free-fermionic character. Although the algebraic structure mirroring the TFIM is used to establish the spectrum, the revised manuscript will include a direct computation showing that the multi-site densities, built from the extraspecial 2-group generators, map to purely bilinear fermionic operators with no surviving quartic or higher terms, owing to the specific relations enforced by the generalized Yang-Baxter construction. revision: yes

  2. Referee: [Conserved quantities paragraph] Section on conserved quantities (the paragraph introducing the local charges that act as background fields): the degeneracy is attributed to these charges, but it is not demonstrated that they commute with the Hamiltonian while remaining independent of the fermionic degrees of freedom that diagonalize the quadratic part. An explicit commutation relation or counting argument establishing that the degeneracy is independent of system size and of the particular choice of R-matrix parameters would strengthen the claim.

    Authors: We will add explicit commutation relations confirming that the local charges commute with the Hamiltonian and are independent of the fermionic modes. A counting argument will also be included demonstrating that the degeneracy is extensive, independent of system size, and holds uniformly across the family of R-matrices obtained from extraspecial 2-groups. revision: yes

Circularity Check

0 steps flagged

No circularity: construction from generalized YBE and group generators is independent of the claimed spectrum

full rationale

The paper derives the multi-site Hamiltonian explicitly from the R-matrix built from extraspecial 2-group generators and the generalized Yang-Baxter equation (citing Rowell-Wang), then separately notes algebraic resemblance to TFIM densities to infer free-fermion solvability and degeneracy from local conserved charges. No equation or claim reduces the spectrum, degeneracy, or thermodynamics to a quantity defined by the result itself, nor does any load-bearing step rely on a self-citation chain or fitted parameter renamed as prediction. The derivation chain remains self-contained against external algebraic inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

The central claim rests on the asserted algebraic resemblance to the transverse-field Ising model and on standard properties of the generalized Yang-Baxter equation; the new element is the specific R-matrix construction.

axioms (1)
  • domain assumption The algebra of its Hamiltonian densities resembles that of the transverse field Ising model
    Invoked to conclude that the spectrum is free-fermionic with degeneracy from local conserved quantities.
invented entities (1)
  • R-matrix constructed using generators of extraspecial 2-groups no independent evidence
    purpose: To satisfy the multi-site generalization of the Yang-Baxter equation and generate the Hamiltonian
    New mathematical object introduced to produce the claimed model and conserved charges.

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Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Symmetries of the Generalized Yang--Baxter Equations

    nlin.SI 2026-06 unverdicted novelty 4.0

    Symmetries of generalized multi-site Yang-Baxter equations depend on site count and frequently outnumber those of the standard equation, heavily constraining inequivalent integrable models.

Reference graph

Works this paper leans on

74 extracted references · 4 linked inside Pith · cited by 1 Pith paper

  1. [1]

    However, it turns out that both H± share the same spectrum

    Closed chain Consider the fermionic Hamiltonians H± = i 2N−1X j=1 ajbj+1 ±ia 2N b1,(35) where±denote periodic and antiperiodic boundary con- ditions, respectively. However, it turns out that both H± share the same spectrum. To see this, consider the operatorγ ε defined as γε = 3X k=1 εkγk, 3X k=1 εkωk = 0, γεaj =−a jγε, γ εbj =−(−1) δj,1bjγε,(36) withj= 1...

  2. [2]

    The split

    Open chain We now briefly talk about the open boundary condi- tion, for which the Hamiltonian becomes Ho = i 2N−1X j=1 ajbj+1 = i 2N−1X j=1 bj ˆCjbj+1.(47) In this case, the degeneracy is enhanced further and be- comes twice as large as only a single sector admits non- trivial spectrum. The boundary modesb 2N , b1, along with the operatorsU kl, suffice to...

  3. [3]

    Crystal statistics. i. a two-dimensional model with an order-disorder transition,

    L. Onsager, “Crystal statistics. i. a two-dimensional model with an order-disorder transition,”Phys. Rev., vol. 65, pp. 117–149, Feb 1944

  4. [4]

    Crystal statistics. ii. partition function 12 Another mapping of such systems to free-fermions can be found in [32]. evaluated by spinor analysis,

    B. Kaufman, “Crystal statistics. ii. partition function 12 Another mapping of such systems to free-fermions can be found in [32]. evaluated by spinor analysis,”Phys. Rev., vol. 76, pp. 1232–1243, Oct 1949

  5. [5]

    Two- dimensional ising model as a soluble problem of many fermions,

    T. D. Schultz, D. C. Mattis, and E. H. Lieb, “Two- dimensional ising model as a soluble problem of many fermions,”Rev. Mod. Phys., vol. 36, pp. 856–871, Jul 1964

  6. [6]

    The one-dimensional ising model with a transverse field,

    P. Pfeuty, “The one-dimensional ising model with a transverse field,”Annals of Physics, vol. 57, no. 1, pp. 79– 90, 1970. 20

  7. [7]

    Two soluble mod- els of an antiferromagnetic chain,

    E. Lieb, T. Schultz, and D. Mattis, “Two soluble mod- els of an antiferromagnetic chain,”Annals of Physics, vol. 16, no. 3, pp. 407–466, 1961

  8. [8]

    A one-way quantum computer,

    R. Raussendorf and H. J. Briegel, “A one-way quantum computer,”Phys. Rev. Lett., vol. 86, pp. 5188–5191, May 2001

  9. [9]

    Quantum phase transition between clus- ter and antiferromagnetic states,

    W. Son, L. Amico, R. Fazio, A. Hamma, S. Pascazio, and V. Vedral, “Quantum phase transition between clus- ter and antiferromagnetic states,”EPL (Europhysics Let- ters), vol. 95, no. 5, p. 50001, 2011

  10. [10]

    ¨Uber das paulische ¨ aquivalenzverbot,

    P. Jordan and E. Wigner, “ ¨Uber das paulische ¨ aquivalenzverbot,”Zeitschrift f¨ ur Physik, vol. 47, no. 9, pp. 631–651, 1928

  11. [11]

    Free fermions in disguise,

    P. Fendley, “Free fermions in disguise,”Journal of Physics A: Mathematical and Theoretical, vol. 52, no. 33, p. 335002, 2019

  12. [12]

    Free fermionic and parafermionic quantum spin chains with multispin inter- actions,

    F. C. Alcaraz and R. A. Pimenta, “Free fermionic and parafermionic quantum spin chains with multispin inter- actions,”Phys. Rev. B, vol. 102, p. 121101(R), Sep 2020

  13. [13]

    Integrable quantum spin chains with free fermionic and parafermionic spec- trum,

    F. C. Alcaraz and R. A. Pimenta, “Integrable quantum spin chains with free fermionic and parafermionic spec- trum,”Phys. Rev. B, vol. 102, p. 235170, Dec 2020

  14. [14]

    Integrable spin chains and cellular automata with medium-range interaction,

    T. Gombor and B. Pozsgay, “Integrable spin chains and cellular automata with medium-range interaction,”Phys. Rev. E, vol. 104, p. 054123, Nov 2021

  15. [15]

    Generalised Onsager Algebra in Quantum Lat- tice Models,

    Y. Miao, “Generalised Onsager Algebra in Quantum Lat- tice Models,”SciPost Phys., vol. 13, p. 070, 2022

  16. [16]

    Dissipative free fermions in disguise,

    K. Fukai, H. Yoshida, and H. Katsura, “Dissipative free fermions in disguise,”ariv:2603.22163 [cond-mat.stat- mech], 2026

  17. [17]

    Free fermions behind the disguise,

    S. J. Elman, A. Chapman, and S. T. Flammia, “Free fermions behind the disguise,”Communications in Math- ematical Physics, vol. 388, no. 2, pp. 969–1003, 2021

  18. [18]

    Characterization of solvable spin models via graph invariants,

    A. Chapman and S. T. Flammia, “Characterization of solvable spin models via graph invariants,”Quantum, vol. 4, p. 278, 2020

  19. [19]

    Geometric criterion for solvability of lattice spin systems,

    M. Ogura, Y. Imamura, N. Kameyama, K. Minami, and M. Sato, “Geometric criterion for solvability of lattice spin systems,”Physical Review B, vol. 102, Dec. 2020

  20. [20]

    Exact real time dynamics with free fermions in disguise,

    I. Vona, M. Mesty´ an, and B. Pozsgay, “Exact real time dynamics with free fermions in disguise,” 2025

  21. [21]

    Construction and simulability of quantum circuits with free fermions in disguise,

    D. Sz´ asz-Schagrin, D. Cristani, L. Piroli, and E. Vernier, “Construction and simulability of quantum circuits with free fermions in disguise,”Quantum Science and Tech- nology, vol. 11, p. 015044, Jan. 2026

  22. [22]

    Classical simula- tion of noninteracting-fermion quantum circuits,

    B. M. Terhal and D. P. DiVincenzo, “Classical simula- tion of noninteracting-fermion quantum circuits,”Physi- cal Review A, vol. 65, Mar. 2002

  23. [23]

    Matchgates and classical sim- ulation of quantum circuits,

    R. Jozsa and A. Miyake, “Matchgates and classical sim- ulation of quantum circuits,”Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sci- ences, vol. 464, no. 2100, p. 3089–3106, 2008

  24. [24]

    Jordan-wigner transformation for quantum- spin systems in two dimensions and fractional statistics,

    E. Fradkin, “Jordan-wigner transformation for quantum- spin systems in two dimensions and fractional statistics,” Phys. Rev. Lett., vol. 63, pp. 322–325, Jul 1989

  25. [25]

    Ground state of the two-dimensional an- tiferromagnetic heisenberg model studied using an ex- tended wigner-jordon transformation,

    Y. R. Wang, “Ground state of the two-dimensional an- tiferromagnetic heisenberg model studied using an ex- tended wigner-jordon transformation,”Phys. Rev. B, vol. 43, pp. 3786(R)–3789(R), Feb 1991

  26. [26]

    Bose-fermi transformation in three-dimensional space,

    L. Huerta and J. Zanelli, “Bose-fermi transformation in three-dimensional space,”Phys. Rev. Lett., vol. 71, pp. 3622–3624, Nov 1993

  27. [27]

    Generalized jordan-wigner transformations,

    C. D. Batista and G. Ortiz, “Generalized jordan-wigner transformations,”Phys. Rev. Lett., vol. 86, pp. 1082– 1085, Feb 2001

  28. [28]

    Arbitrary di- mensional majorana dualities and architectures for topo- logical matter,

    Z. Nussinov, G. Ortiz, and E. Cobanera, “Arbitrary di- mensional majorana dualities and architectures for topo- logical matter,”Phys. Rev. B, vol. 86, p. 085415, Aug 2012

  29. [29]

    Jordan– wigner transformations for tree structures,

    S. Backens, A. Shnirman, and Y. Makhlin, “Jordan– wigner transformations for tree structures,”Scientific Reports, vol. 9, no. 1, p. 2598, 2019

  30. [30]

    Mapping local hamiltoni- ans of fermions to local hamiltonians of spins,

    F. Verstraete and J. I. Cirac, “Mapping local hamiltoni- ans of fermions to local hamiltonians of spins,”Journal of Statistical Mechanics: Theory and Experiment, vol. 2005, p. P09012, sep 2005

  31. [31]

    Exact bosonization in two spatial dimensions and a new class of lattice gauge theories,

    Y.-A. Chen, A. Kapustin, and D. Radicevi´ c, “Exact bosonization in two spatial dimensions and a new class of lattice gauge theories,”Annals of Physics, vol. 393, pp. 234–253, 2018

  32. [32]

    Jordan-wigner dualities for translation-invariant hamiltonians in any dimension: Emergent fermions in fracton topological order,

    N. Tantivasadakarn, “Jordan-wigner dualities for translation-invariant hamiltonians in any dimension: Emergent fermions in fracton topological order,” Physical Review Research, vol. 2, no. 2, 2020

  33. [33]

    Bonsai algorithm: Grow your own fermion-to-qubit mappings,

    A. Miller, Z. Zimbor´ as, S. Knecht, S. Maniscalco, and G. Garc´ ıa-P´ erez, “Bonsai algorithm: Grow your own fermion-to-qubit mappings,”PRX Quantum, vol. 4, p. 030314, Aug 2023

  34. [34]

    Solvable hamiltonians and fermionization transformations obtained from operators satisfying spe- cific commutation relations,

    K. Minami, “Solvable hamiltonians and fermionization transformations obtained from operators satisfying spe- cific commutation relations,”Journal of the Physical So- ciety of Japan, vol. 85, no. 2, p. 024003, 2016

  35. [35]

    Quantum Inverse Scattering Method and Correlation Functions,

    V. E. Korepin, N. M. Bogoliubov, and A. G. Izergin, “Quantum Inverse Scattering Method and Correlation Functions,” Cambridge university press, 1993

  36. [36]

    Ex- traspecial two-groups, generalized yang-baxter equations and braiding quantum gates,

    E. C. Rowell, Y. Zhang, Y.-S. Wu, and M.-L. Ge, “Ex- traspecial two-groups, generalized yang-baxter equations and braiding quantum gates,” 2010

  37. [37]

    Quan- tum entanglement, supersymmetry, and the generalized yang-baxter equation.,

    P. Padmanabhan, F. Sugino, and D. Trancanelli, “Quan- tum entanglement, supersymmetry, and the generalized yang-baxter equation.,”Quantum Information and Com- putation, 2019

  38. [38]

    The Yang–Baxter integrability of the critical Ising chain,

    A. Sinha, T. Justin, P. Padmanabhan, and V. Kore- pin, “The Yang–Baxter integrability of the critical Ising chain,”J. Stat. Mech., vol. 2025, no. 10, p. 103102, 2025

  39. [39]

    Lectures on yangian symmetry,

    F. Loebbert, “Lectures on yangian symmetry,”Jour- nal of Physics A: Mathematical and Theoretical, vol. 49, no. 32, p. 323002, 2016

  40. [40]

    Ising model with four-spin interactions,

    F. W. Wu, “Ising model with four-spin interactions,” Phys. Rev. B, vol. 4, pp. 2312–2314, Oct 1971

  41. [41]

    Duality in generalized ising models,

    F. J. Wegner, “Duality in generalized ising models,” arXiv:1411.5815 [hep-lat], 2014

  42. [42]

    Duality in generalized ising models and phase transitions without local order parameters,

    F. J. Wegner, “Duality in generalized ising models and phase transitions without local order parameters,”Jour- nal of Mathematical Physics, vol. 12, pp. 2259–2272, 10 1971

  43. [43]

    Ising analogs of quantum spin chains with multispin interac- tions,

    F. C. Alcaraz, R. A. Pimenta, and J. Sirker, “Ising analogs of quantum spin chains with multispin interac- tions,”Physical Review B, vol. 107, no. 23, 2023

  44. [44]

    Extraspe- cial 2-groups and images of braid group representations,

    J. M. Franko, E. C. Rowell, and Z. Wang, “Extraspe- cial 2-groups and images of braid group representations,” Journal of Knot Theory and Its Ramifications, vol. 15, no. 04, pp. 413–427, 2006

  45. [45]

    Anyons in an exactly solved model and be- yond,

    A. Kitaev, “Anyons in an exactly solved model and be- yond,”Annals of Physics, vol. 321, no. 1, pp. 2–111, 2006. January Special Issue

  46. [46]

    The hilbert-space structure of 21 free fermions in disguise,

    E. Vernier and L. Piroli, “The hilbert-space structure of 21 free fermions in disguise,”Journal of Statistical Mechan- ics: Theory and Experiment, vol. 2026, no. 1, p. 013101, 2026

  47. [47]

    Takahashi,Thermodynamics of One-Dimensional Solvable Models

    M. Takahashi,Thermodynamics of One-Dimensional Solvable Models. Cambridge University Press, 1999

  48. [48]

    Statistical mechanics of the x y model. ii. spin-correlation functions,

    E. Barouch and B. M. McCoy, “Statistical mechanics of the x y model. ii. spin-correlation functions,”Physical Review A, vol. 3, pp. 786–804, 1971

  49. [49]

    Time- dependent correlation functions of the transverse ising chain at the critical magnetic field,

    B. M. McCoy, J. H. Perk, and R. E. Shrock, “Time- dependent correlation functions of the transverse ising chain at the critical magnetic field,”Nuclear Physics B, vol. 220, no. 1, pp. 35–47, 1983

  50. [50]

    Lattice models in statistical mechanics and soliton equations,

    B. M. McCoy, “Lattice models in statistical mechanics and soliton equations,” 1993

  51. [51]

    Lieb-robinson correlation function for the quantum transverse-field ising model,

    B. J. Mahoney and C. S. Lent, “Lieb-robinson correlation function for the quantum transverse-field ising model,” Physical Review Research, vol. 6, no. 2, 2024

  52. [52]

    New results for the correlation functions of the ising model and the trans- verse ising chain,

    J. H. H. Perk and H. Au-Yang, “New results for the correlation functions of the ising model and the trans- verse ising chain,”Journal of Statistical Physics, vol. 135, p. 599–619, May 2009

  53. [53]

    Quench dynamics and relaxation in isolated integrable quantum spin chains,

    F. H. L. Essler and M. Fagotti, “Quench dynamics and relaxation in isolated integrable quantum spin chains,” Journal of Statistical Mechanics: Theory and Experi- ment, vol. 2016, no. 6, p. 064002, 2016

  54. [54]

    Temperature correlations of quantum spins,

    A. R. Its, A. G. Izergin, V. E. Korepin, and N. A. Slavnov, “Temperature correlations of quantum spins,” Physical Review Letters, vol. 70, p. 1704–1706, Mar. 1993

  55. [55]

    On the equivalence of the discrete non- linear schr¨ odinger equation and the discrete isotropic heisenberg magnet,

    T. Hoffmann, “On the equivalence of the discrete non- linear schr¨ odinger equation and the discrete isotropic heisenberg magnet,”Physics Letters A, vol. 265, p. 62–67, Jan. 2000

  56. [56]

    Differential Equations for Quantum Cor- relation Functions,

    A. R. Its, A. G. Izergin, V. E. Korepin, and N. A. Slavnov, “Differential Equations for Quantum Cor- relation Functions,”International Journal of Modern Physics B, vol. 4, pp. 1003–1037, Jan. 1990

  57. [57]

    Algebraic classification of hietarinta’s solutions of yang- baxter equations: invertible 4×4 operators,

    S. Maity, V. K. Singh, P. Padmanabhan, and V. Korepin, “Algebraic classification of hietarinta’s solutions of yang- baxter equations: invertible 4×4 operators,”Journal of High Energy Physics, vol. 2024, no. 12, p. 67, 2024

  58. [58]

    Integrability of a family of clean syk models from the critical ising chain,

    K. Fukai and H. Katsura, “Integrability of a family of clean syk models from the critical ising chain,”Phys. Rev. B, vol. 113, p. 115107, Mar 2026

  59. [59]

    Boost operator and its applica- tion to quantum gelfand-levitan equation for heisenberg- ising chain with spin one-half,

    K. Sogo and M. Wadati, “Boost operator and its applica- tion to quantum gelfand-levitan equation for heisenberg- ising chain with spin one-half,”Progress of Theoretical Physics, vol. 69, no. 2, pp. 431–450, 1983

  60. [60]

    Infinite set of conserved charges in the ising model,

    M. Grady, “Infinite set of conserved charges in the ising model,”Physical Review D, vol. 25, no. 4, p. 1103, 1982

  61. [61]

    Conserved charges of series of solvable lat- tice models,

    K. Minami, “Conserved charges of series of solvable lat- tice models,”Nuclear Physics B, vol. 1012, p. 116844, 2025

  62. [62]

    Statistics of the two-dimensional ferromagnet. part i,

    H. A. Kramers and G. H. Wannier, “Statistics of the two-dimensional ferromagnet. part i,”Phys. Rev., vol. 60, pp. 252–262, Aug 1941

  63. [63]

    Statistics of the two- dimensional ferromagnet. part ii,

    H. A. Kramers and G. H. Wannier, “Statistics of the two- dimensional ferromagnet. part ii,”Phys. Rev., vol. 60, pp. 263–276, Aug 1941

  64. [64]

    Topological defects on the lattice: I. the ising model,

    D. Aasen, R. S. Mong, and P. Fendley, “Topological defects on the lattice: I. the ising model,”Journal of Physics A: Mathematical and Theoretical, vol. 49, no. 35, p. 354001, 2016

  65. [65]

    Topological de- fects on the lattice: dualities and degeneracies,

    D. Aasen, P. Fendley, and R. S. Mong, “Topological de- fects on the lattice: dualities and degeneracies,”arXiv preprint arXiv:2008.08598, 2020

  66. [66]

    Majorana chain and ising model-(non-invertible) translations, anomalies, and em- anant symmetries,

    N. Seiberg and S.-H. Shao, “Majorana chain and ising model-(non-invertible) translations, anomalies, and em- anant symmetries,”SciPost Physics, vol. 16, no. 3, p. 064, 2024

  67. [67]

    Non- invertible Kramers-Wannier duality-symmetry in the trotterized critical Ising chain,

    A. Sinha, P. Padmanabhan, and V. Korepin, “Non- invertible Kramers-Wannier duality-symmetry in the trotterized critical Ising chain,” 11 2025

  68. [68]

    Braid- ing quantum gates from partition algebras,

    P. Padmanabhan, F. Sugino, and D. Trancanelli, “Braid- ing quantum gates from partition algebras,”Quantum, vol. 4, p. 311, Aug. 2020

  69. [69]

    Gen- erating w states with braiding operators,

    P. Padmanabhan, F. Sugino, and D. Trancanelli, “Gen- erating w states with braiding operators,”arXiv preprint arXiv:2007.05660, 2020

  70. [70]

    Topological aspects of quantum entanglement,

    L. H. Kauffman and E. Mehrotra, “Topological aspects of quantum entanglement,”arXiv:1611.08047[math.GT], 2018

  71. [71]

    Braiding operators are universal quantum gates,

    L. H. Kauffman and S. J. Lomonaco, “Braiding operators are universal quantum gates,”New Journal of Physics, vol. 6, p. 134–134, Oct. 2004

  72. [72]

    Generalized yang-baxter equations and braid- ing quantum gates,

    R. Chen, “Generalized yang-baxter equations and braid- ing quantum gates,”arXiv:1108.5215[math.QA], 2011

  73. [73]

    Yang–baxter operators need quantum entanglement to distinguish knots,

    G. Alagic, M. Jarret, and S. P. Jordan, “Yang–baxter operators need quantum entanglement to distinguish knots,”Journal of Physics A: Mathematical and Theo- retical, vol. 49, p. 075203, Jan. 2016

  74. [74]

    Qubit rep- resentations of the braid groups from generalized yang- baxter matrices,

    J. F. Vasquez, Z. Wang, and H. M. Wong, “Qubit rep- resentations of the braid groups from generalized yang- baxter matrices,”arXiv:1602.08536[math.QA], 2016. Appendix A: Review of the(d, l, m)-gYBE We denote the generalizedR-matrix withlindices as, R1···l({u})≡R j1···jl({u}) ;{u}= (u 1,· · ·, u l)∈C.(A1) In this notation, the (d, l, m)-gYBE reads, R1···l(...