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arxiv: 2605.06079 · v1 · submitted 2026-05-07 · 🧮 math-ph · math.CA· math.MP

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Accessory Parameter of Confluent Heun Equations, Voros Periods and classical irregular conformal blocks

Ayato Shukuta, Hajime Nagoya, Kohei Iwaki

Pith reviewed 2026-05-08 04:35 UTC · model grok-4.3

classification 🧮 math-ph math.CAmath.MP
keywords accessory parameterconfluent Heun equationVoros periodclassical conformal blockirregular singularityspectral curvecycle selectionformal series expansion
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The pith

The accessory parameters of confluent Heun equations admit formal series expansions in Voros periods that match classical conformal blocks when cycles are chosen appropriately.

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

This paper derives formal series expansions of the accessory parameters for the Heun differential equation and all of its confluent versions by employing Voros periods. These expansions are compared with classical conformal blocks to test whether the relation between periods and blocks continues to hold when singularities are irregular. The authors supply an explicit prescription for selecting cycles on the spectral curve so that the Voros period reproduces the accessory parameter linked to the conformal block.

Core claim

For the Heun differential equation and all of its confluent equations, formal series expansions of the accessory parameters are derived using the Voros periods. These expansions are compared with the classical conformal blocks, and the Zamolodchikov-type conjecture is examined for irregular singularities. In particular, a detailed prescription is provided for choosing cycles on the spectral curve that yield the Voros period which corresponds to the classical (regular or irregular) conformal blocks through the accessory parameter.

What carries the argument

The Voros period associated with a chosen cycle on the spectral curve, which generates the formal series expansion of the accessory parameter and thereby links it to the classical conformal block.

Load-bearing premise

The Zamolodchikov-type conjecture holds between the Voros periods and the classical conformal blocks even for irregular singularities, and the chosen cycles produce the matching accessory parameter without additional corrections.

What would settle it

Computing the first few coefficients in the formal series for an accessory parameter from Voros periods on a specific irregular confluent Heun equation and finding that they differ from the coefficients in the corresponding classical conformal block expansion would falsify the claimed correspondence.

read the original abstract

For the Heun differential equation and all of its confluent equations, we derive formal series expansions of the accessory parameters using the Voros periods. We then compare these expansions with the classical conformal blocks recently obtained by Bonelli--Shchechkin--Tanzini, and examine the Zamolodchikov-type conjecture expected to hold between them, allowing for irregular singularities. In particular, as an extension of the previous works of Mironov--Morozov, Piatek--Pietrykowski and Lisovyy--Naidiuk, we provide a detailed prescription for choosing cycles on the spectral curve that yield the Voros period which corresponds to the classical (regular or irregular) conformal blocks through the accessory parameter.

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 manuscript derives formal series expansions for the accessory parameters of the Heun equation and all its confluent forms by means of Voros periods on the associated spectral curve. These expansions are compared with the classical conformal blocks recently obtained by Bonelli–Shchechkin–Tanzini; the Zamolodchikov-type conjecture relating the two quantities is examined in the presence of irregular singularities. A detailed prescription is supplied for the choice of cycles on the spectral curve that are asserted to produce the Voros period corresponding to the (regular or irregular) classical conformal blocks via the accessory parameter. The work extends earlier results of Mironov–Morozov, Piatek–Pietrykowski and Lisovyy–Naidiuk.

Significance. If the cycle prescription and the resulting series are rigorously justified, the paper would furnish a concrete computational bridge between the WKB/Voros formalism and the classical irregular conformal blocks, extending the regular-singularity correspondence to the confluent cases. The explicit cycle-selection rules constitute a useful technical contribution that could be applied to accessory-parameter computations in integrable systems and related conformal-field-theory contexts.

major comments (2)
  1. [Sections presenting the cycle prescription and the comparison with BST expansions] The central claim that the prescribed cycles yield Voros periods matching the BST classical blocks for irregular singularities rests on the assumption that the Zamolodchikov-type relation continues to hold without additional Stokes or monodromy corrections. However, the manuscript does not supply an explicit base-case verification for the simplest irregular confluent equation (e.g., the confluent Heun equation) in which higher-order coefficients of the derived series are shown to agree with independent BST expansions beyond the leading orders already known from the regular-singularity literature.
  2. [Derivation of the formal series expansions] The formal series are stated to be derived from the Voros periods, yet the text does not clarify whether the WKB expansion is carried out to all orders or truncated, nor does it address possible resurgence or Stokes phenomena that could affect the identification of the accessory parameter for irregular singularities.
minor comments (2)
  1. Notation for the spectral curve, the chosen cycles, and the precise definition of the Voros period should be introduced with a single, self-contained paragraph early in the manuscript to aid readability.
  2. A short table summarizing the leading coefficients obtained from the Voros method versus the BST expansions for at least one irregular case would make the comparison more transparent.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address the two major comments point by point below, indicating the revisions we intend to incorporate.

read point-by-point responses
  1. Referee: [Sections presenting the cycle prescription and the comparison with BST expansions] The central claim that the prescribed cycles yield Voros periods matching the BST classical blocks for irregular singularities rests on the assumption that the Zamolodchikov-type relation continues to hold without additional Stokes or monodromy corrections. However, the manuscript does not supply an explicit base-case verification for the simplest irregular confluent equation (e.g., the confluent Heun equation) in which higher-order coefficients of the derived series are shown to agree with independent BST expansions beyond the leading orders already known from the regular-singularity literature.

    Authors: We agree that an explicit higher-order verification for the simplest irregular case would make the central claim more robust. In the revised manuscript we will add a new subsection that computes the accessory-parameter series for the confluent Heun equation up to order four using the prescribed cycles and directly compares the coefficients with the corresponding terms of the BST expansion. This will provide the requested base-case check beyond the orders already known from the regular-singularity literature. revision: yes

  2. Referee: [Derivation of the formal series expansions] The formal series are stated to be derived from the Voros periods, yet the text does not clarify whether the WKB expansion is carried out to all orders or truncated, nor does it address possible resurgence or Stokes phenomena that could affect the identification of the accessory parameter for irregular singularities.

    Authors: The expansions are formal power series obtained from the all-order WKB analysis of the Voros periods; they are not truncated. We will revise the relevant sections to state this explicitly and to display the general recursive structure of the coefficients. With regard to resurgence and Stokes phenomena, the present work focuses on the formal identification of the accessory parameter via the cycle prescription. A complete treatment of Stokes jumps and their possible effect on the accessory-parameter identification lies beyond the scope of this paper and would require exact-WKB techniques that we do not develop here. revision: partial

standing simulated objections not resolved
  • A full analysis of resurgence and Stokes phenomena for the irregular confluent cases and their possible impact on the accessory-parameter identification.

Circularity Check

0 steps flagged

No circularity: accessory series derived from independent Voros period analysis on spectral curve; comparison tests conjecture without reduction to inputs

full rationale

The derivation begins with the confluent Heun equation and constructs formal series for its accessory parameter directly from Voros periods, which are contour integrals over cycles on the associated spectral curve. This step uses standard asymptotic/WKB techniques on the curve and does not presuppose the value of the accessory parameter or the conformal-block expansions. The paper then compares the resulting series to the independent Bonelli–Shchechkin–Tanzini expansions and examines whether the Zamolodchikov-type relation continues to hold for irregular singularities. The cycle prescription is presented as an explicit extension of earlier literature (Mironov–Morozov et al.) rather than a definition that forces the match. No equation or step reduces the claimed output to a fitted input, self-citation, or tautological renaming; the central chain remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; no explicit free parameters, axioms, or invented entities can be extracted from the provided text.

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Reference graph

Works this paper leans on

43 extracted references · 36 canonical work pages

  1. [1]

    L. F. Alday, D. Gaiotto, and Y. Tachikawa, Liouville correlation functions from four-dimensional gauge theories,Lett. Math. Phys.91(2010), 167–197; doi.org/10.1007/s11005-010-0369-5, arXiv:0906.3219 [hep-th]

  2. [2]

    Aminov, A

    G. Aminov, A. Grassi, and Y. Hatsuda, Black Hole Quasinormal Modes and Seiberg–Witten Theory,Annales Henri Poincar´ e,23(2022), 1951–1977; 10.1007/s00023-021-01137-x. arXiv:2006.06111 [hep-th]

  3. [3]

    Bershtein and A

    M. Bershtein and A. Shchechkin,Bilinear equations on Painlev´ eτfunctions from CFT, Commun. Math. Phys.339(2015), 1021–1061; doi:10.1007/s00220-015-2427-4, arXiv:1406.3008 [math-ph]

  4. [4]

    Bershtein, P

    M. Bershtein, P. Gavrylenko and A. Marshakov, Cluster integrable systems, q-Painlev´ e equations and their quantization, Journal of High Energy Physics2018, no. 02, 077 (2018), doi:10.1007/JHEP02(2018)077. arXiv:1711.02063 [math-ph]

  5. [5]

    Bonelli, O

    G. Bonelli, O. Lisovyy, K. Maruyoshi, A. Sciarappa, and A. Tanzini, On Painlev´ e/gauge theory correspondence,Lett. Math. Phys.107(2017), 2359–2413, arXiv:1612.06235 [hep-th]

  6. [6]

    Bonelli, A

    G. Bonelli, A. Shchechkin and A. Tanzini, Refined Painlev´ e/gauge theory correspondence and quantum tau functions, arXiv:2502.01499 [hep-th]

  7. [7]

    Bonelli, A

    G. Bonelli, A. Shchechkin, and A. Tanzini, Bilinearτ-forms of quantum Painlev´ e equations andC 2/Z2 blowup relations in SUSY gauge theories, arXiv:2512.25051 [math-ph]

  8. [8]

    Delabaere, H

    E. Delabaere, H. Dillinger and F. Pham, R´ esurgence de Voros et p´ eriodes des courbes hyperelliptiques,Annales de l’Institut Fourier (Grenoble)49(1999), no. 1, 211–253

  9. [9]

    Desiraju, P

    H. Desiraju, P. Ghosal, and A. Prokhorov, Proof of Zamolodchikov conjecture for semi-classical conformal blocks on the torus, arXiv:2407.05839 [hep-th]

  10. [10]

    Gaiotto, Asymptotically freeN= 2 theories and irregular conformal blocks,J

    D. Gaiotto, Asymptotically freeN= 2 theories and irregular conformal blocks,J. Phys. Conf. Ser.462(2013), 012014, arXiv:0908.0307 [hep-th]

  11. [11]

    Gaiotto and J

    D. Gaiotto and J. Teschner, Irregular singularities in Liouville theory, doi:10.48550/arXiv.1203.1052, arXiv:1203.1052 [hep- th]

  12. [12]

    Gamayun, N

    O. Gamayun, N. Iorgov, and O. Lisovyy, Conformal field theory of Painlev´ e VI,J. High Energy Phys.2012, no. 10, 038, arXiv:1207.0787 [hep-th]

  13. [13]

    Gamayun, N

    O. Gamayun, N. Iorgov, and O. Lisovyy, How instanton combinatorics solves Painlev´ e VI, V and III’s,J. Phys. A: Math. Theor.46(2013), 335203, arXiv:1302.1832 [hep-th]

  14. [14]

    Gavrylenko, A

    P. Gavrylenko, A. Marshakov, and A. Stoyan, Irregular conformal blocks, Painlev´ e III and the blow-up equations,Journal of High Energy Physics,2020, no. 12, 125 (2020); doi:10.1007/JHEP12(2020)125, arXiv:2006.15652 [math-ph]

  15. [15]

    Grassi, J

    A. Grassi, J. Gu and M. Mari˜ no, Non-perturbative approaches to the quantum Seiberg–Witten curve,J. High Energ. Phys., 2020, 106 (2020); doi.org/10.1007/JHEP07(2020)106, arXiv:1908.07065 [hep-th]

  16. [16]

    Grassi, Q

    A. Grassi, Q. Hao and A. Neitzke, Exact WKB methods inSU(2)N f = 1,J. High Energ. Phys. 2022, 46 (2022); doi.org/10.1007/JHEP01(2022)046, arXiv:2105.03777 [hep-th]

  17. [17]

    Gu amd M

    J. Gu amd M. Mari˜ no, On the resurgent structure of quantum periodsSciPost Phys.,15, 035 (2023); doi:10.21468/SciPostPhys.15.1.035. arXiv:2211.03871 [hep-th]

  18. [18]

    Hatsuda, Quasinormal modes of Kerr-de Sitter black holes via the Heun function,Class

    Y. Hatsuda, Quasinormal modes of Kerr-de Sitter black holes via the Heun function,Class. Quant. Grav.38(2020) no.2, 025015; doi:10.1088/1361-6382/abc82e, arXiv:2006.08957 [gr-qc]

  19. [19]

    Iorgov, K

    N. Iorgov, K. Iwaki, O. Lisovyy, and Y. Zhuravlov, Many-faced Painlev´ e I: irregular conformal blocks, topological recursion, and holomorphic anomaly approaches, arXiv:2505.16803 [math-ph]

  20. [20]

    Iwaki, 2-Parameterτ-Function for the First Painlev´ e Equation: Topological Recursion and Direct Monodromy Problem via Exact WKB Analysis,Commun

    K. Iwaki, 2-Parameterτ-Function for the First Painlev´ e Equation: Topological Recursion and Direct Monodromy Problem via Exact WKB Analysis,Commun. Math. Phys.,377(2020), 1047–1098. arXiv:1902.06439 [math-ph]

  21. [21]

    Iwaki, Les Houches Lectures on Exact WKB Analysis and Painlev´ e Equations, arXiv:2512.17599 [math-ph]

    K. Iwaki, Les Houches Lectures on Exact WKB Analysis and Painlev´ e Equations, arXiv:2512.17599 [math-ph]

  22. [22]

    Iwaki, T

    K. Iwaki, T. Koike and Y.-M. Takei, Voros Coefficients for the Hypergeometric Differential Equations and Eynard-Orantin’s Topological Recursion – Part II : For the Confluent Family of Hypergeometric Equations, Journal of Integrable Systems,4 (2019), xyz004; arXiv:1810.02946 [math.CA]

  23. [23]

    Iwaki and T

    K. Iwaki and T. Nakanishi, Exact WKB analysis and cluster algebras, J. Phys. A: Math. Theor.,47(2014), 474009; arXiv:1401.7094 [math.CA]

  24. [24]

    Kawai and Y

    T. Kawai and Y. Takei,Algebraic Analysis of Singular Perturbation Theory, Transl. Math. Monogr.227, Amer. Math. Soc, 2005

  25. [25]

    Lisovyy and A

    O. Lisovyy and A. Naidiuk, Accessory parameters in confluent Heun equations and classical irregular conformal blocks, Letters in Mathematical Physics,111(2021). arXiv:2101.05715 [math-ph]

  26. [26]

    Mironov and A

    A. Mironov and A. Morozov, Nekrasov Functions and Exact Bohr–Sommerfeld Integrals,J. High Energy Phys.2010 (2010), 40, arXiv:0910.5670 [hep-th]

  27. [27]

    Nagoya, Quantum Painlev´ e systems of typeA (1) l ,Int

    H. Nagoya, Quantum Painlev´ e systems of typeA (1) l ,Int. J. Math.15 (2004), no. 10, 1007–1031, arXiv:math/0402281 [math.QA]

  28. [28]

    Nagoya, Irregular conformal blocks, with an application to the fifth and fourth Painlev´ e equations,J

    H. Nagoya, Irregular conformal blocks, with an application to the fifth and fourth Painlev´ e equations,J. Math. Phys.,56 (2015), 123505; arXiv:1505.02398 [math-ph]

  29. [29]

    H. Nagoya, Remarks on irregular conformal blocks and Painlev´ e III and II tau functions,Proceedings of the Meeting for Study of Number theory, Hopf Algebras and Related Topics, Yokohama Publishers, 2019, 105–124. arXiv:1804.04782

  30. [30]

    N. A. Nekrasov and S. L. Shatashvili, Quantization of integrable systems and four-dimensional gauge theories, arXiv:0908.4052 [hep-th]. ACCESSORY PARAMETER, VOROS PERIODS AND CLASSICAL CONFORMAL BLOCKS 49

  31. [31]

    Novaes and B

    F. Novaes and B. Carneiro da Cunha, Isomonodromy, Painlev´ e transcendents and scattering off of black holes,J. High Energy Phys.2014, no. 07, 132, arXiv:1404.5188 [hep-th]

  32. [32]

    Novaes, C

    F. Novaes, C. Marinho, M. Lencs´ es, and M. Casals, Kerr–de Sitter quasinormal modes via accessory parameter expansion, J. High Energy Phys.2019 (2019), 33, doi:10.1007/JHEP05(2019)033, arXiv:1811.11912 [gr-qc]

  33. [33]

    K. Osuga, Deformation and quantisation condition of theQ-top recursion,Annales Henri Poincar´ e,25, 4033–4064 (2024); https://doi.org/10.1007/s00023-024-01421-6, arXiv:2307.02112 [math-ph]

  34. [34]

    Piatek and A

    M. Piatek and A. R. Pietrykowski, Classical irregular block,N= 2 pure gauge theory and Mathieu equation,J. High Energy Phys.2014 (2014), 32, arXiv:1407.0305 [hep-th]

  35. [35]

    Piatek and A

    M. Piatek and A. R. Pietrykowski, Classical irregular blocks, Hill’s equation andPT-symmetric periodic complex potentials, J. High Energy Phys.2016 (2016), 131, arXiv:1604.03574 [hep-th]

  36. [36]

    Poghosyan and R

    H. Poghosyan and R. Poghossian, A note on rank 5/2 Liouville irregular block, Painlev´ e I and theH 0 Argyres–Douglas theory,J. High Energy Phys.2023 (2023), 198, arXiv:2308.09623 [hep-th]

  37. [37]

    Rim and H

    C. Rim and H. Zhang, Classical Virasoro irregular conformal block,J. High Energy Phys.2015 (2015), 163, arXiv:1504.07910 [hep-th]

  38. [38]

    Rim and H

    C. Rim and H. Zhang, Classical Virasoro irregular conformal block II,J. High Energy Phys.2015 (2015), 97, arXiv:1506.03561 [hep-th]

  39. [39]

    M. Sato, T. Aoki, T. Kawai and Y. Takei, Algebraic analysis of singular perturbations (in Japanese; written by A. Kaneko), RIMS Kˆ okyˆ uroku,750(1991), 43–51

  40. [40]

    S. Yu. Slavyanov and W. Lay,Special functions: a unified theory based on singularities, Oxford University Press, 2000

  41. [41]

    Voros, The return of the quartic oscillator

    A. Voros, The return of the quartic oscillator. The complex WKB method,Annals of the IHP Theoretical Physics,39 (1983), 211–338

  42. [42]

    M. Wakayama, Equivalence between the eigenvalue problem of non-commutative harmonic oscillators and existence of holomorphic solutions of Heun’s differential equations, eigenstates degeneration, and Rabi’s model,Int. Math. Res. Not. IMRN(2016), 759–794

  43. [43]

    A. B. Zamolodchikov, Two-dimensional conformal symmetry and critical four-spin correlation functions in the Ashkin-Teller model.Soviet Journal of Experimental and Theoretical Physics,63(1986), 1061–1066. Graduate School of Mathematical Sciences, The University of Tokyo, Japan Email address:k-iwaki@g.ecc.u-tokyo.ac.jp School of Mathematics and Physics, Kan...