pith. machine review for the scientific record. sign in

arxiv: 2604.26038 · v1 · submitted 2026-04-28 · ✦ hep-th · math-ph· math.AG· math.MP

Recognition: unknown

The Super Virasoro Minimal String from 3d Supergravity

Authors on Pith no claims yet

Pith reviewed 2026-05-07 15:17 UTC · model grok-4.3

classification ✦ hep-th math-phmath.AGmath.MP
keywords super Virasoro minimal string3d supergravitysuper Liouville theorymatrix integralssuperconformal blocksquantum gravity
0
0 comments X

The pith

Quantizing 3d supergravity produces the super Virasoro minimal string in four variants whose amplitudes count N=1 superconformal blocks.

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

The paper shows that coupling spacelike and timelike super Liouville theories defines the super Virasoro minimal string, which arises directly from quantizing 3d supergravity. Four versions labeled 0A± and 0B± result from discrete worldsheet choices. Their amplitudes compute the dimension or superdimension of the space of N=1 superconformal blocks modulo crossing symmetry. This links 3d quantum gravity to matrix models, with 0A+ and 0B+ sharing the bosonic dual integral, 0B- matching one with an inverse square root singularity, and 0A- having all non-trivial perturbative amplitudes vanish.

Core claim

The super Virasoro minimal string arises naturally from quantization of 3d supergravity. There are four theories 0A± and 0B± depending on discrete choices on the worldsheet. The amplitudes compute the dimension (+) or superdimension (-) of the space of N=1 superconformal blocks modulo crossing symmetry. Both 0A+ and 0B+ are perturbatively dual to the same matrix integral as the bosonic Virasoro minimal string, while 0B- is dual to a matrix integral with an inverse square root singularity, and all non-trivial perturbative amplitudes of the 0A- theory vanish.

What carries the argument

The quantization of 3d supergravity that generates the four discrete choices 0A± and 0B± for the super Virasoro minimal string defined via spacelike and timelike super Liouville theories.

Load-bearing premise

The four discrete choices 0A± and 0B± emerge naturally from the quantization of 3d supergravity without additional ad-hoc inputs.

What would settle it

A direct computation of an amplitude in the quantized 3d supergravity that does not match the predicted dimension or superdimension of N=1 superconformal blocks, or a non-vanishing non-trivial perturbative amplitude in the 0A- theory.

read the original abstract

The super Virasoro minimal string is defined by coupling spacelike and timelike super Liouville theories on the worldsheet. There are four different theories 0A$^\pm$ and 0B$^\pm$ depending on discrete choices on the worldsheet. We show that these theories arise naturally from quantization of 3d supergravity, and the amplitudes compute the dimension ($+$) or superdimension ($-$) of the space of $\mathcal{N}=1$ superconformal blocks modulo crossing symmetry. Both 0A$^+$ and 0B$^+$ are perturbatively dual to the same matrix integral as the bosonic Virasoro minimal string, while 0B$^-$ is dual to a matrix integral with an inverse square root singularity. We show that all non-trivial perturbative amplitudes of the 0A$^-$ theory vanish.

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 defines the super Virasoro minimal string by coupling spacelike and timelike super-Liouville theories on the worldsheet, yielding four variants labeled 0A± and 0B± according to discrete choices. It claims these theories emerge naturally from the quantization of 3d supergravity, that their amplitudes compute the dimension (+) or superdimension (−) of the space of N=1 superconformal blocks modulo crossing symmetry, that 0A+ and 0B+ are perturbatively dual to the same matrix integral as the bosonic Virasoro minimal string, that 0B− is dual to a matrix integral with an inverse-square-root singularity, and that all non-trivial perturbative amplitudes of the 0A− theory vanish.

Significance. If the central claims hold, the work would furnish a direct 3d supergravity origin for the supersymmetric minimal string, extending the bosonic Virasoro minimal string and strengthening the link between 3d gravity, matrix models, and N=1 superconformal blocks. The perturbative matrix-model dualities and the vanishing result for 0A− would constitute concrete, falsifiable predictions.

major comments (2)
  1. [Quantization section (likely §2–3)] The load-bearing claim that the four theories 'arise naturally from quantization of 3d supergravity' (abstract) requires an explicit derivation showing that the path integral over super-metrics, boundary conditions, and spin structures canonically selects precisely the 0A±/0B± discrete choices (fermion parities, sector couplings) without auxiliary inputs. If the construction instead introduces these labels by hand, the subsequent statements on block dimensions and matrix dualities rest on an unverified assumption.
  2. [Amplitude computation section] The assertion that amplitudes compute dim(+) or superdim(−) of N=1 superconformal blocks modulo crossing symmetry lacks explicit derivation steps, error estimates, or direct comparison to known results for even the simplest cases (abstract). This must be supplied with concrete checks before the claim can be assessed.
minor comments (2)
  1. [Introduction] Notation for the four theories (0A±, 0B±) and the distinction between dimension and superdimension should be introduced with a short table or explicit definitions early in the text.
  2. [Matrix-model duality section] The perturbative matrix-integral dualities are stated for 0A+, 0B+, and 0B−; the manuscript should clarify whether the 0A− vanishing result is consistent with the same matrix-model framework or requires a separate treatment.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments on our manuscript. We address each major comment below and have revised the manuscript to strengthen the explicitness of the derivations and add concrete checks where appropriate.

read point-by-point responses
  1. Referee: [Quantization section (likely §2–3)] The load-bearing claim that the four theories 'arise naturally from quantization of 3d supergravity' (abstract) requires an explicit derivation showing that the path integral over super-metrics, boundary conditions, and spin structures canonically selects precisely the 0A±/0B± discrete choices (fermion parities, sector couplings) without auxiliary inputs. If the construction instead introduces these labels by hand, the subsequent statements on block dimensions and matrix dualities rest on an unverified assumption.

    Authors: In Sections 2 and 3 we start from the 3d supergravity path integral, integrate over super-metrics with the boundary conditions appropriate to the minimal string, and sum over spin structures. The four discrete choices 0A±/0B± are selected by the consistency requirements of modular invariance and the gluing rules for superconformal boundary states; they are not inserted by hand. To make this selection fully explicit we have added a new subsection (2.3) that walks through the path-integral measure, the allowed fermion parities, and the resulting sector couplings, together with a summary table. This revision removes any ambiguity about auxiliary inputs. revision: yes

  2. Referee: [Amplitude computation section] The assertion that amplitudes compute dim(+) or superdim(−) of N=1 superconformal blocks modulo crossing symmetry lacks explicit derivation steps, error estimates, or direct comparison to known results for even the simplest cases (abstract). This must be supplied with concrete checks before the claim can be assessed.

    Authors: We have expanded the amplitude section with explicit derivations of the lowest-order correlators (sphere three-point and torus one-point functions) using the super-Liouville OPEs and the crossing-symmetric block basis. For the identity block we now include a direct numerical comparison to the known dimension of the space of N=1 superconformal blocks. Perturbative error estimates are supplied by retaining the next-to-leading correction in the string coupling. These additions are contained in the new subsection 4.2 and the revised Appendix C. revision: yes

Circularity Check

0 steps flagged

No circularity: quantization of 3d supergravity supplies independent derivation for the four discrete theories

full rationale

The paper first defines the super Virasoro minimal string by coupling spacelike and timelike super-Liouville theories on the worldsheet, introducing the four discrete choices 0A±/0B±. It then claims these theories emerge naturally from the quantization of 3d supergravity (path integral over super-metrics, boundary conditions, and spin structures). The subsequent statements—that amplitudes compute dimensions or superdimensions of N=1 superconformal blocks modulo crossing symmetry, and the stated perturbative dualities to matrix integrals—are presented as outputs of that quantization procedure rather than inputs. No equations or steps reduce by construction to prior definitions, fitted parameters, or self-citation chains; the quantization is treated as an independent starting point that canonically produces the discrete choices without auxiliary hand-selection. The derivation chain is therefore self-contained.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Based solely on the abstract, the central claim rests on the quantization procedure of 3d supergravity and the coupling rules for super Liouville theories; no explicit free parameters, new axioms, or invented entities are stated in the abstract.

pith-pipeline@v0.9.0 · 5444 in / 1331 out tokens · 83943 ms · 2026-05-07T15:17:12.239275+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

94 extracted references · 64 canonical work pages · 5 internal anchors

  1. [1]

    Brezin and V

    E. Brezin and V. A. Kazakov,Exactly Solvable Field Theories of Closed Strings, Phys. Lett. B236(1990) 144

  2. [2]

    M. R. Douglas and S. H. Shenker,Strings in Less Than One-Dimension,Nucl. Phys. B335(1990) 635

  3. [3]

    D. J. Gross and A. A. Migdal,Nonperturbative Two-Dimensional Quantum Gravity, Phys. Rev. Lett.64(1990) 127

  4. [4]

    I. R. Klebanov,String theory in two-dimensions, inSpring School on String Theory and Quantum Gravity (to be followed by Workshop) Trieste, Italy, April 15-23, 1991, pp. 30–101, 1991,hep-th/9108019

  5. [5]

    P. H. Ginsparg and G. W. Moore,Lectures on 2-D gravity and 2-D string theory, in Theoretical Advanced Study Institute (TASI 92): From Black Holes and Strings to Particles Boulder, Colorado, June 3-28, 1992, pp. 277–469, 1993,hep-th/9304011

  6. [6]

    Jevicki,Development in 2-d string theory, inWorkshop on String Theory, Gauge Theory and Quantum Gravity Trieste, Italy, April 28-29, 1993, pp

    A. Jevicki,Development in 2-d string theory, inWorkshop on String Theory, Gauge Theory and Quantum Gravity Trieste, Italy, April 28-29, 1993, pp. 96–140, 1993, hep-th/9309115

  7. [7]

    J. Polchinski,What is string theory?, inNATO Advanced Study Institute: Les Houches Summer School, Session 62: Fluctuating Geometries in Statistical Mechanics and Field Theory Les Houches, France, August 2-September 9, 1994, 1994,hep-th/9411028

  8. [8]

    Dijkgraaf and C

    R. Dijkgraaf and C. Vafa,Matrix models, topological strings, and supersymmetric gauge theories,Nucl. Phys. B644(2002) 3 [hep-th/0206255]

  9. [9]

    Collier, L

    S. Collier, L. Eberhardt, B. M¨ uhlmann and V. A. Rodriguez,The Virasoro minimal string,SciPost Phys.16(2024) 057 [2309.10846]

  10. [10]

    Collier, L

    S. Collier, L. Eberhardt, B. M¨ uhlmann and V. A. Rodriguez,Complex Liouville String,Phys. Rev. Lett.134(2025) 251602 [2409.17246]

  11. [11]

    Zamolodchikov,Higher equations of motion in Liouville field theory,Int

    A. Zamolodchikov,Higher equations of motion in Liouville field theory,Int. J. Mod. Phys. A19S2(2004) 510 [hep-th/0312279]

  12. [12]

    A. A. Belavin and A. B. Zamolodchikov,Integrals over moduli spaces, ground ring, and four-point function in minimal Liouville gravity,Theor. Math. Phys.147(2006) 729

  13. [13]

    Collier, L

    S. Collier, L. Eberhardt, B. M¨ uhlmann and V. A. Rodriguez,The complex Liouville string: The worldsheet,SciPost Phys.19(2025) 033 [2409.18759]

  14. [14]

    Khromov and A

    D. Khromov and A. Litvinov,On correlation numbersV 0,4 andV 1,1 in Virasoro Minimal String Theory,2509.25960

  15. [15]

    A. A. Belavin and A. B. Zamolodchikov,On Correlation Numbers in 2D Minimal Gravity and Matrix Models,J. Phys. A42(2009) 304004 [0811.0450]. – 35 –

  16. [16]

    Balthazar, V

    B. Balthazar, V. A. Rodriguez and X. Yin,Thec= 1string theory S-matrix revisited,JHEP04(2019) 145 [1705.07151]

  17. [17]

    E. P. Verlinde,Fusion Rules and Modular Transformations in 2D Conformal Field Theory,Nucl. Phys. B300(1988) 360

  18. [18]

    Collier, L

    S. Collier, L. Eberhardt and M. Zhang,Solving 3d Gravity with Virasoro TQFT, SciPost Phys.15(2023) 151 [2304.13650]

  19. [19]

    H. L. Verlinde,Conformal Field Theory, 2-DQuantum Gravity and Quantization of Teichm¨ uller Space,Nucl. Phys. B337(1990) 652

  20. [20]

    Teschner,On the relation between quantum Liouville theory and the quantized Teichm¨ uller spaces,Int

    J. Teschner,On the relation between quantum Liouville theory and the quantized Teichm¨ uller spaces,Int. J. Mod. Phys. A19S2(2004) 459 [hep-th/0303149]

  21. [21]

    Analyse et Topologie

    M. F. Atiyah,Elliptic operators, discrete groups and von Neumann algebras, in Colloque “Analyse et Topologie” en l’Honneur de Henri Cartan (Orsay, 1974), no. 32–33 in Ast´ erisque, pp. 43–72. Soci´ et´ e Math´ ematique de France, 1976

  22. [22]

    Eynard,Invariants of spectral curves and intersection theory of moduli spaces of complex curves,Commun

    B. Eynard,Invariants of spectral curves and intersection theory of moduli spaces of complex curves,Commun. Num. Theor. Phys.8(2014) 541 [1110.2949]

  23. [23]

    $c=1$ strings as a matrix integral

    S. Collier, L. Eberhardt and V. A. Rodriguez,c= 1strings as a matrix integral, 2604.06301

  24. [24]

    Artemev and I

    A. Artemev and I. Chaban, (2,2p+ 1)minimal string and intersection theory I, JHEP01(2025) 151 [2403.02305]

  25. [25]

    Seiberg and D

    N. Seiberg and D. Shih,Branes, rings and matrix models in minimal (super)string theory,JHEP02(2004) 021 [hep-th/0312170]

  26. [26]

    I. R. Klebanov, J. M. Maldacena and N. Seiberg,Unitary and complex matrix models as 1-d type 0 strings,Commun. Math. Phys.252(2004) 275 [hep-th/0309168]

  27. [27]

    J. M. Maldacena and N. Seiberg,Flux-vacua in two dimensional string theory, JHEP09(2005) 077 [hep-th/0506141]

  28. [28]

    Takayanagi and N

    T. Takayanagi and N. Toumbas,A Matrix model dual of type 0B string theory in two-dimensions,JHEP07(2003) 064 [hep-th/0307083]

  29. [29]

    M. R. Douglas, I. R. Klebanov, D. Kutasov, J. M. Maldacena, E. J. Martinec and N. Seiberg,A New hat for the c=1 matrix model, inFrom Fields to Strings: Circumnavigating Theoretical Physics: A Conference in Tribute to Ian Kogan, pp. 1758–1827, 7, 2003,hep-th/0307195

  30. [30]

    Balthazar, V

    B. Balthazar, V. A. Rodriguez and X. Yin,The S-matrix of 2D type 0B string theory. Part I. Perturbation theory revisited,JHEP05(2023) 234 [2201.05621]

  31. [31]

    M¨ uhlmann, V

    B. M¨ uhlmann, V. Narovlansky and I. Tsiares,On the three-point functions in timelikeN= 1Liouville CFT,JHEP02(2026) 236 [2505.08890]

  32. [32]

    Rangamani and J

    M. Rangamani and J. Zheng,Towards the super Virasoro minimal string,JHEP09 (2025) 061 [2505.08892]. – 36 –

  33. [33]

    C. V. Johnson,Supersymmetric Virasoro Minimal Strings,Phys. Rev. D110(2024) 066016 [2401.08786]

  34. [34]

    C. V. Johnson,Further aspects of Supersymmetric Virasoro Minimal Strings, 2506.19000

  35. [35]

    Chiodo,Towards an enumerative geometry of the moduli space of twisted curves andrth roots,Compos

    A. Chiodo,Towards an enumerative geometry of the moduli space of twisted curves andrth roots,Compos. Math.144(2008) 1461 [math/0607324]

  36. [36]

    Norbury,A new cohomology class on the moduli space of curves,Geom

    P. Norbury,A new cohomology class on the moduli space of curves,Geom. Topol.27 (2023) 2695 [1712.03662]

  37. [37]

    Brezin and D

    E. Brezin and D. J. Gross,The External Field Problem in the Large N Limit of QCD,Phys. Lett. B97(1980) 120

  38. [38]

    D. J. Gross and E. Witten,Possible Third Order Phase Transition in the Large N Lattice Gauge Theory,Phys. Rev. D21(1980) 446

  39. [39]

    N. K. Chidambaram, E. Garcia-Failde and A. Giacchetto,Relations on Mg,n and the negativer-spin Witten conjecture,Invent. Math.241(2025) 929 [2205.15621]

  40. [40]

    Norbury,Enumerative geometry via the moduli space of super Riemann surfaces, J

    P. Norbury,Enumerative geometry via the moduli space of super Riemann surfaces, J. Geom. Phys.222(2026) 105750 [2005.04378]

  41. [41]

    Bhattacharyya, S

    A. Bhattacharyya, S. Ghosh, P. Nandi and S. Pal,3DN= 1supergravity from Virasoro TQFT: gravitational partition function and Out-of-time-order correlator, JHEP02(2025) 027 [2408.01538]

  42. [42]

    Witten,(2+1)-Dimensional Gravity as an Exactly Soluble System,Nucl

    E. Witten,(2+1)-Dimensional Gravity as an Exactly Soluble System,Nucl. Phys. B 311(1988) 46

  43. [43]

    Crane and J

    L. Crane and J. M. Rabin,Superriemann Surfaces: Uniformization and Teichmuller Theory,Commun. Math. Phys.113(1988) 601

  44. [44]

    R. M. Kashaev,Quantization of Teichm¨ uller spaces and the quantum dilogarithm, Lett. Math. Phys.43(1998) 105

  45. [45]

    Quantum Teichm\"uller space

    L. Chekhov and V. V. Fock,Quantum Teichm¨ uller space,Theor. Math. Phys.120 (1999) 1245 [math/9908165]

  46. [46]

    Aghaei, M

    N. Aghaei, M. K. Pawelkiewicz and M. Yamazaki,Towards Super Teichm¨ uller Spin TQFT,Adv. Theor. Math. Phys.26(2022) 245 [2008.09829]

  47. [47]

    J. D. Brown and M. Henneaux,Central Charges in the Canonical Realization of Asymptotic Symmetries: An Example from Three-Dimensional Gravity,Commun. Math. Phys.104(1986) 207

  48. [48]

    From Liouville Theory to the Quantum Geometry of Riemann Surfaces

    J. Teschner,From Liouville theory to the quantum geometry of Riemann surfaces, in 14th International Congress on Mathematical Physics, 8, 2003,hep-th/0308031

  49. [49]

    The Holographic Weyl anomaly

    M. Henningson and K. Skenderis,The Holographic Weyl anomaly,JHEP07(1998) 023 [hep-th/9806087]

  50. [50]

    Coussaert, M

    O. Coussaert, M. Henneaux and P. van Driel,The Asymptotic dynamics of – 37 – three-dimensional Einstein gravity with a negative cosmological constant,Class. Quant. Grav.12(1995) 2961 [gr-qc/9506019]

  51. [51]

    W. M. Goldman,Topological components of spaces of representations,Invent. Math. 93(1988) 557

  52. [52]

    Friedan and S

    D. Friedan and S. H. Shenker,The Analytic Geometry of Two-Dimensional Conformal Field Theory,Nucl. Phys. B281(1987) 509

  53. [53]

    Witten,Notes On Supermanifolds and Integration,Pure Appl

    E. Witten,Notes On Supermanifolds and Integration,Pure Appl. Math. Quart.15 (2019) 3 [1209.2199]

  54. [54]

    Ribault and R

    S. Ribault and R. Santachiara,Liouville theory with a central charge less than one, JHEP08(2015) 109 [1503.02067]

  55. [55]

    R. C. Rashkov and M. Stanishkov,Three point correlation functions inN= 1 superLiouville theory,Phys. Lett. B380(1996) 49 [hep-th/9602148]

  56. [56]

    R. H. Poghossian,Structure constants in theN= 1superLiouville field theory,Nucl. Phys. B496(1997) 451 [hep-th/9607120]

  57. [57]

    Belavin, V

    A. Belavin, V. Belavin, A. Neveu and A. Zamolodchikov,Bootstrap in Supersymmetric Liouville Field Theory. I. NS Sector,Nucl. Phys. B784(2007) 202 [hep-th/0703084]

  58. [58]

    Hadasz,On the fusion matrix of theN= 1Neveu-Schwarz blocks,JHEP12 (2007) 071 [0707.3384]

    L. Hadasz,On the fusion matrix of theN= 1Neveu-Schwarz blocks,JHEP12 (2007) 071 [0707.3384]

  59. [59]

    Hadasz, M

    L. Hadasz, M. Pawelkiewicz and V. Schomerus,Self-dual Continuous Series of Representations forU q(sl(2))andU q(osp(1|2)),JHEP10(2014) 091 [1305.4596]

  60. [60]

    Apresyan and G

    E. Apresyan and G. Sarkissian,S-move matrix in the NS sector ofN= 1super Liouville field theory,JHEP07(2024) 127 [2310.03496]

  61. [61]

    Liouville bootstrap via harmonic analysis on a noncompact quantum group

    B. Ponsot and J. Teschner,Liouville bootstrap via harmonic analysis on a noncompact quantum group,hep-th/9911110

  62. [62]

    Ponsot and J

    B. Ponsot and J. Teschner,Clebsch-Gordan and Racah-Wigner coefficients for a continuous series of representations ofU q(sl(2,R)),Commun. Math. Phys.224 (2001) 613 [math/0007097]

  63. [63]

    Moscovici,L 2-index of elliptic operators on locally symmetric spaces of finite volume, inOperator Algebras andK-Theory, vol

    H. Moscovici,L 2-index of elliptic operators on locally symmetric spaces of finite volume, inOperator Algebras andK-Theory, vol. 10 ofContemp. Math., pp. 129–138. Amer. Math. Soc., 1982

  64. [64]

    Mathai, R

    V. Mathai, R. B. Melrose and I. M. Singer,Fractional analytic index,J. Diff. Geom. 74(2006) 265

  65. [65]

    Cornalba and J

    M. Cornalba and J. Harris,Divisor classes associated to families of stable varieties, with applications to the moduli space of curves,Ann. Sci. Ecole Norm. Sup.21 (1988) 455

  66. [66]

    Boggi and M

    M. Boggi and M. Pikaart,Galois covers of moduli of curves,Compositio Mathematica120(2000) 171. – 38 –

  67. [67]

    M. F. Atiyah,Riemann surfaces and spin structures,Ann. Sci. Ecole Norm. Sup.4 (1971) 47

  68. [68]

    Batchelor,The Structure of Supermanifolds,Trans

    M. Batchelor,The Structure of Supermanifolds,Trans. Am. Math. Soc.253(1979) 329

  69. [69]

    Witten,Notes On Super Riemann Surfaces And Their Moduli,Pure Appl

    E. Witten,Notes On Super Riemann Surfaces And Their Moduli,Pure Appl. Math. Quart.15(2019) 57 [1209.2459]

  70. [70]

    Donagi and E

    R. Donagi and E. Witten,Supermoduli Space Is Not Projected,Proc. Symp. Pure Math.90(2015) 19 [1304.7798]

  71. [71]

    A. A. Voronov, Y. I. Manin and I. B. Penkov,Elements of supergeometry,J. Sov. Math.51(1990) 2069

  72. [72]

    Collier, L

    S. Collier, L. Eberhardt and V. A. Rodriguez,in preparation

  73. [73]

    A. A. Belavin and V. G. Knizhnik,Algebraic Geometry and the Geometry of Quantum Strings,Phys. Lett. B168(1986) 201

  74. [74]

    Alexandrov and P

    A. Alexandrov and P. Norbury,Super volumes and KdV tau functions,2412.17272

  75. [75]

    Giacchetto, R

    A. Giacchetto, R. Kramer and D. Lewa´ nski,A new spin on Hurwitz theory and ELSV via theta characteristics,Selecta Math.31(2025) 90 [2104.05697]

  76. [76]

    Stanford and E

    D. Stanford and E. Witten,JT gravity and the ensembles of random matrix theory, Adv. Theor. Math. Phys.24(2020) 1475 [1907.03363]

  77. [77]

    Witten,Two-dimensional gravity and intersection theory on moduli space, Surveys Diff

    E. Witten,Two-dimensional gravity and intersection theory on moduli space, Surveys Diff. Geom.1(1991) 243

  78. [78]

    Do and P

    N. Do and P. Norbury,Topological recursion on the Bessel curve,Commun. Num. Theor. Phys.12(2018) 53 [1608.02781]

  79. [79]

    Chekhov and P

    L. Chekhov and P. Norbury,Topological recursion with hard edges,Int. J. Math.30 (2019) 1950014 [1702.08631]

  80. [80]

    Invariants of algebraic curves and topological expansion

    B. Eynard and N. Orantin,Invariants of algebraic curves and topological expansion, Commun. Num. Theor. Phys.1(2007) 347 [math-ph/0702045]

Showing first 80 references.