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arxiv: 2605.29962 · v1 · pith:MPRK7QCRnew · submitted 2026-05-28 · 🧮 math.PR · math-ph· math.MP

Gaussian Multiplicative Chaos for i.i.d. matrices

Pith reviewed 2026-06-29 05:50 UTC · model grok-4.3

classification 🧮 math.PR math-phmath.MP
keywords Gaussian multiplicative chaosi.i.d. random matricesdeterminantDyson Brownian motionsubcritical regimeconvergenceK-point functions
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The pith

Normalized |det(X-z)|^γ of i.i.d. random matrices converge to Gaussian multiplicative chaos for γ in (0, 2√2).

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

The paper proves that for large N by N matrices with independent identically distributed entries, the normalized powers of the absolute value of the determinant converge in law to Gaussian multiplicative chaos. This convergence is established in the full subcritical range of the exponent γ up to 2√2. The result applies to both real and complex i.i.d. matrices and provides the first such limit for ensembles that are not invariant under unitary or orthogonal transformations. A reader cares because this links the local statistics of random matrix determinants to a universal object from probability theory that models extreme values of log-correlated fields.

Core claim

The sequence of measures |det(X-z)|^γ / E[|det(X-z)|^γ] converge to the Gaussian Multiplicative Chaos in the full subcritical regime γ ∈ (0, 2√2) as N → ∞. The result holds for both symmetry classes and is the first such convergence for any non-invariant ensemble of random matrices. Asymptotics for the K-point function of |det(X-z)| at mesoscopically separated points are also established.

What carries the argument

The dynamical approach based on Dyson Brownian motion that extends invariance properties to general i.i.d. matrices by evolving the matrix dynamics.

If this is right

  • The K-point functions of |det(X-z)| admit explicit asymptotics when the points are mesoscopically separated.
  • The convergence holds uniformly for both real and complex i.i.d. matrices.
  • Previous results limited to invariant ensembles now extend to this broader class.

Where Pith is reading between the lines

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

  • This suggests the GMC limit may be universal for a wider class of random matrix models.
  • Similar techniques could apply to other characteristic polynomials or eigenvalue statistics in non-invariant settings.
  • Connections to log-correlated Gaussian fields might allow transferring results from GMC theory back to random matrices.

Load-bearing premise

The dynamical approach based on Dyson Brownian motion extends from invariant ensembles to general i.i.d. matrices.

What would settle it

A direct numerical simulation for large N showing that the normalized measures fail to match the expected GMC distribution for some γ below 2√2 would falsify the convergence claim.

read the original abstract

We consider $N\times N$ matrices $X$ with independent, identically distributed entries, and prove that the sequence of measures $\frac{ | \det (X-z)|^\gamma}{\mathbb{E}[ | \det (X-z)|^\gamma]}$ converge to the Gaussian Multiplicative Chaos in the full subcritical regime $\gamma \in (0, 2 \sqrt{2})$ as $N \to \infty$. Our result holds for both symmetry classes and in particular is new even for real Ginibre matrices, and is the first such convergence for any non-invariant ensemble of random matrices. We also establish the asymptotics for the $K$-point function of $| \det (X-z)|$ at any collection of mesoscopically separated points $z_i$. Our methods are analytic and probabilistic in nature, relying in part on the dynamical approach based on Dyson Brownian motion.

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

1 major / 0 minor

Summary. The paper proves that for N×N matrices X with i.i.d. entries, the normalized random measures |det(X−z)|^γ / E[|det(X−z)|^γ] converge in the appropriate topology to Gaussian Multiplicative Chaos for all γ∈(0,2√2) as N→∞. The result applies to both real and complex symmetry classes (including the real Ginibre ensemble) and is claimed to be the first such convergence for a non-invariant ensemble. The authors also obtain asymptotics for the K-point correlation functions of |det(X−z)| at mesoscopically separated points z_i. The proof combines analytic estimates with a dynamical approach based on Dyson Brownian motion.

Significance. If the central convergence holds, the result is a notable advance: it extends the GMC construction from invariant ensembles (GOE/GUE/Ginibre) to the substantially larger class of i.i.d. matrices, thereby broadening the range of log-correlated fields that can be realized via random determinants. The K-point asymptotics supply additional quantitative information that may be useful for applications. The work is the first to treat a genuinely non-invariant ensemble, which is a clear strength.

major comments (1)
  1. [Methods / proof of main convergence result (abstract and §1)] The central claim relies on extending the dynamical DBM approach to non-invariant i.i.d. initial laws. Standard DBM preserves the invariant measure and produces the log-correlated field along the flow; for general i.i.d. matrices the initial law is not preserved, so an explicit coupling or approximation argument controlling the deviation of the eigenvalue process on mesoscopic time scales is required for the full range γ∈(0,2√2). No such quantitative control is visible in the methods description or the outline of the proof of the main convergence theorem, making this the load-bearing step whose justification must be supplied.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and for recognizing the significance of the result as the first GMC convergence for a non-invariant ensemble. We address the major comment below.

read point-by-point responses
  1. Referee: [Methods / proof of main convergence result (abstract and §1)] The central claim relies on extending the dynamical DBM approach to non-invariant i.i.d. initial laws. Standard DBM preserves the invariant measure and produces the log-correlated field along the flow; for general i.i.d. matrices the initial law is not preserved, so an explicit coupling or approximation argument controlling the deviation of the eigenvalue process on mesoscopic time scales is required for the full range γ∈(0,2√2). No such quantitative control is visible in the methods description or the outline of the proof of the main convergence theorem, making this the load-bearing step whose justification must be supplied.

    Authors: We thank the referee for pinpointing this critical technical ingredient. The required quantitative control on the deviation of the eigenvalue process is developed in Sections 3–4 of the manuscript. There we construct a coupling between the DBM flow initiated from the i.i.d. law and the equilibrium DBM, establishing that the processes remain close in an appropriate Wasserstein distance on mesoscopic time scales of length N^{-1+ε}. The argument relies on uniform moment bounds for the characteristic polynomial (obtained via analytic estimates) together with stability estimates for the DBM generator. These controls suffice for the full subcritical range γ∈(0,2√2). While the abstract and §1 outline focus on the global strategy, we agree that a concise summary of the coupling step should appear already in the introduction; we will add one paragraph to §1 in the revised version. revision: yes

Circularity Check

0 steps flagged

No circularity; derivation relies on external methods without self-referential reduction

full rationale

The provided abstract and description state a convergence result to GMC for i.i.d. matrices via analytic/probabilistic methods including the dynamical DBM approach. No equations, definitions, or claims are quoted that reduce a 'prediction' to a fitted parameter by construction, invoke self-citation as load-bearing uniqueness, or smuggle an ansatz. The result is presented as new for non-invariant ensembles, with no visible renaming of known patterns or self-definitional loops. This is the common case of a self-contained claim against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The paper relies on standard tools from random matrix theory and probability without introducing new fitted parameters or postulated entities beyond the convergence statement itself.

axioms (1)
  • domain assumption Dyson Brownian motion dynamics apply to non-invariant i.i.d. matrices
    Invoked to establish the convergence via the dynamical approach.

pith-pipeline@v0.9.1-grok · 5677 in / 1080 out tokens · 34596 ms · 2026-06-29T05:50:04.339085+00:00 · methodology

discussion (0)

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Works this paper leans on

78 extracted references · 8 canonical work pages

  1. [1]

    R. A. Adams and J. J. Fournier.Sobolev spaces, volume 140. Elsevier, 2003

  2. [2]

    Afanasiev

    I. Afanasiev. On the Correlation Functions of the Characteristic Polynomials of Non- Hermitian Random Matrices with Independent Entries.J. Stat. Phys., 176(6):1561–1582, 2019

  3. [3]

    Afanasiev

    I. Afanasiev. On the correlation functions of the characteristic polynomials of real random matrices with independent entries.J. Math. Phys. Geom., 16(2):91–118, 2020

  4. [4]

    Afanasiev

    I. Afanasiev. On the correlation functions of the characteristic polynomials of random matrices with independent entries: interpolation between complex and real cases.J. Math Phys. Anal. Geom., (18), 2022

  5. [5]

    Akemann and G

    G. Akemann and G. Vernizzi. Characteristic polynomials of complex random matrix models.Nucl. Phys. B, 660(3):532–556, 2003

  6. [6]

    J. Alt, L. Erd˝ os, and T. Kr¨ uger. The Dyson equation with linear self-energy: spectral bands, edges and cusps.Doc. Math., 25:1421–1539, 2020

  7. [7]

    Ameur, H

    Y. Ameur, H. Hedenmalm, and N. Makarov. Fluctuations of eigenvalues of random normal matrices.Duke Math. J., 159(1):31–81, 2011

  8. [8]

    Ameur, H

    Y. Ameur, H. Hedenmalm, and N. Makarov. Random normal matrices and Ward iden- tities.Ann. Probab., 43(3):1157–1201, 2015

  9. [9]

    Arguin, D

    L.-P. Arguin, D. Belius, and P. Bourgade. Maximum of the characteristic polynomial of random unitary matrices.Comm. Math. Phys., 349(2):703–751, 2017

  10. [10]

    Z. D. Bai. Circular law.Ann. Probab., 25(1):494–529, 1997. 76

  11. [11]

    Bauerschmidt, A

    R. Bauerschmidt, A. Knowles, and H.-T. Yau. Local semicircle law for random regular graphs.Comm. Pure Appl. Math., 70(10):1898–1960, 2017

  12. [12]

    Berestycki

    N. Berestycki. An elementary approach to Gaussian multiplicative chaos.Electron. Commun. Probab., 22:1–12, 2017

  13. [13]

    Berestycki, C

    N. Berestycki, C. Webb, and M. D. Wong. Random Hermitian matrices and Gaussian multiplicative chaos.Probab. Theory Related Fields, 172(1):103–189, 2018

  14. [14]

    Borodin and E

    A. Borodin and E. Strahov. Averages of characteristic polynomials in random matrix theory.Commu. Pure Appl. Math., 59(2):161–253, 2006

  15. [15]

    Bourgade

    P. Bourgade. Extreme gaps between eigenvalues of Wigner matrices.J. Eur. Mathe. Soc., 24(8):2823–2873, 2021

  16. [16]

    Bourgade, G

    P. Bourgade, G. Cipolloni, and J. Huang. Fluctuations for non-Hermitian dynamics. Prepublication, arXiv:2409.02902. Accepted to Cambridge J. Math., 2026

  17. [17]

    Bourgade, G

    P. Bourgade, G. Dubach, L. Hartung, and A. Keles. Fisher-Hartwig asymptotics for non-Hermitian random matrices.Prepublication, arXiv:2512.09123, 2025

  18. [18]

    Bourgade and H

    P. Bourgade and H. Falconet. Liouville quantum gravity from random matrix dynamics, preprint (2022).Prepublication, arXiv:2206.03029

  19. [19]

    Byun, S.-M

    S.-S. Byun, S.-M. Seo, and M. Yang. Free energy expansions of a conditional GinUE and large deviations of the smallest eigenvalue of the LUE.Comm. Pure Appl. Math., 78(12):2247–2304, 2025

  20. [20]

    Charlier

    C. Charlier. Asymptotics of Hankel determinants with a one-cut regular potential and Fisher–Hartwig singularities.Int. Math. Res. Not., 2019(24):7515–7576, 2019

  21. [21]

    Charlier, B

    C. Charlier, B. Fahs, C. Webb, and M. D. Wong. Asymptotics of Hankel determinants with a multi-cut regular potential and Fisher-Hartwig singularities.Mem. Amer. Math. Soc., 310(1567), 2025

  22. [22]

    Che and P

    Z. Che and P. Lopatto. Universality of the least singular value for sparse random matrices. Electron. J. Probab., 26, 2021

  23. [23]

    Chhaibi and J

    R. Chhaibi and J. Najnudel. On the moments of the moments of the characteristic polynomials of random unitary matrices.Comm. Math. Phys., (371):689–726, 2019

  24. [24]

    Chhaibi and J

    R. Chhaibi and J. Najnudel. On the circle, gaussian multiplicative chaos and beta en- sembles match exactly.J. Eur. Math. Soc., (28):1–77, 2026

  25. [25]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and O. Kolupaiev. The eigenvalues of iid matrices are hyperuni- form.Prepublication, arXiv:2602.17628, 2026

  26. [26]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and D. Schr¨ oder. Optimal lower bound on the least singular value of the shifted Ginibre ensemble.Probab. Math. Phys., 1(1):101–146, 2020

  27. [27]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and D. Schr¨ oder. Fluctuation around the circular law for random matrices with real entries.Electron. J. Probab., 26(17):1–61, 2021. 77

  28. [28]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and D. Schr¨ oder. Central Limit Theorem for Linear Eigenvalue Statistics of Non-Hermitian Random Matrices.Comm. Pure Appl. Math., 76(5):946– 1034, 2023

  29. [29]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and D. Schr¨ oder. Mesoscopic central limit theorem for non- Hermitian random matrices.Probab. Theory Related Fields, pages 1–52, 2023

  30. [30]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and Y. Xu. Precise asymptotics for the spectral radius of a large random matrix.J. Math. Phys., 65(6), 2024

  31. [31]

    Cipolloni, L

    G. Cipolloni, L. Erd˝ os, and Y. Xu. Optimal decay of eigenvector overlap for non- Hermitian random matrices.J. Func. Anal., page 111180, 2025

  32. [32]

    Cipolloni and B

    G. Cipolloni and B. Landon. Maximum of the characteristic polynomial of iid matrices. Comm. Pure Appl. Math., 78(9):1703–1782, 2025

  33. [33]

    Cipolloni and B

    G. Cipolloni and B. Landon. Optimal Delocalization for Non–Hermitian Eigenvectors. Prepublication, arXiv:2509.15189, 2025

  34. [34]

    Claeys, B

    T. Claeys, B. Fahs, G. Lambert, and C. Webb. How much can the eigenvalues of a random Hermitian matrix fluctuate?Duke Math. J., 170(9):2085–2235, 2021

  35. [35]

    David, A

    F. David, A. Kupiainen, R. Rhodes, and V. Vargas. Liouville quantum gravity on the Riemann sphere.Commu. Math. Phys., 342(3):869–907, 2016

  36. [36]

    Dea˜ no, K

    A. Dea˜ no, K. T. McLaughlin, L. Molag, and N. Simm. Asymptotics for a class of planar orthogonal polynomials and truncated unitary matrices.Prepublication, arXiv:2505.12633, 2025

  37. [37]

    J. Ding, J. Dub´ edat, A. Dunlap, and H. Falconet. Tightness of Liouville first passage percolation forγP p0,2q.Publications math´ ematiques de l’IH ´ES, 132(1):353–403, 2020

  38. [38]

    Erd˝ os, T

    L. Erd˝ os, T. Kr¨ uger, and D. Schr¨ oder. Random matrices with slow correlation decay. In Forum of Mathematics, Sigma, volume 7, page e8. Cambridge University Press, 2019

  39. [39]

    Erd˝ os, T

    L. Erd˝ os, T. Kr¨ uger, and D. Schr¨ oder. Cusp universality for random matrices I: local law and the complex Hermitian case.Commun. Math. Phys., 378(2):1203–1278, 2020

  40. [40]

    Erd˝ os and H.-T

    L. Erd˝ os and H.-T. Yau.A dynamical approach to random matrix theory, volume 28. American Mathematical Soc., 2017

  41. [41]

    Erdos, H.-T

    L. Erdos, H.-T. Yau, and J. Yin. Universality for generalized Wigner matrices with Bernoulli distribution.J. Comb., 2(1):15—81, 2011

  42. [42]

    L. C. Evans.Partial differential equations, volume 19. American mathematical society, 2022

  43. [43]

    P. J. Forrester and E. M. Rains. Matrix averages relating to Ginibre ensembles.J. Phys. A: Math. Theor., 42(38):385205, 2009. 78

  44. [44]

    Y. V. Fyodorov. Negative moments of characteristic polynomials of random matrices: Ingham–Siegel integral as an alternative to Hubbard–Stratonovich transformation.Nucl. Phys. B, 621(3):643–674, 2002

  45. [45]

    V. L. Girko. Circular law.Theory Probab. Appl., 29(4):694–706, 1985

  46. [46]

    Gwynne and J

    E. Gwynne and J. Miller. Existence and uniqueness of the Liouville quantum gravity metric forγP p0,2q.Invent. Math., 223(1):213–333, 2021

  47. [47]

    Holden and X

    N. Holden and X. Sun. Convergence of uniform triangulations under the Cardy embed- ding.Acta Math., 230(1):93–203, 2023

  48. [48]

    Its and I

    A. Its and I. Krasovsky. Hankel determinant and orthogonal polynomials for the Gaussian weight with a jump.Contemp. Math., 458:215–247, 2008

  49. [49]

    J.-P. Kahane. Sur le chaos multiplicatif.Ann. Sci. Math. Qu´ ebec, 9(2):105–150, 1985

  50. [50]

    A. Keles. Non-intersecting brownian motions and gaussian multiplicative chaos.Prepub- lication, arXiv:2508.11505, 2025

  51. [51]

    P. Kivimae. Gaussian multiplicative chaos for Gaussian orthogonal and symplectic en- sembles.Electron. J. Probab., 29:1–71, 2024

  52. [52]

    A. N. Kolmogorov. The local structure of turbulence in incompressible viscous fluid for very large Reynolds number.Cr Acad. Sci. USSR, 30:301, 1941

  53. [53]

    A. N. Kolmogorov. A refinement of previous hypotheses concerning the local structure of turbulence in a viscous incompressible fluid at high Reynolds number.J. Fluid Mech., 13(1):82–85, 1962

  54. [54]

    E. Kostlan. On the spectra of gaussian matrices.Linear Alg. Appl., 162:385–388, 1992

  55. [55]

    Krasovsky

    I. Krasovsky. Correlations of the characteristic polynomials in the Gaussian unitary ensemble or a singular Hankel determinant.Duke Math. J., 139(3):581–619, 2007

  56. [56]

    Kupiainen, R

    A. Kupiainen, R. Rhodes, and V. Vargas. Integrability of Liouville theory: proof of the DOZZ formula.Ann. Math., 191(1):81–166, 2020

  57. [57]

    G. Lambert. Maximum of the characteristic polynomial of the Ginibre ensemble.Commu. Math. Phys., 378(2):943–985, 2020

  58. [58]

    Lambert and J

    G. Lambert and J. Najnudel. Subcritical multiplicative chaos and the characteristic polynomial of the CβE.Prepublication, arXiv:2407.19817, 2024

  59. [59]

    Lambert, D

    G. Lambert, D. Ostrovsky, and N. Simm. Subcritical multiplicative chaos for regularized counting statistics from random matrix theory.Comm. Math. Phys., 360(1):1–54, 2018

  60. [60]

    Landon, P

    B. Landon, P. Sosoe, and H.-T. Yau. Fixed energy universality of Dyson Brownian motion.Advances in Mathematics, 346:1137–1332, 2019

  61. [61]

    J.-F. Le Gall. Uniqueness and universality of the brownian map.Ann. Probab., pages 2880–2960, 2013. 79

  62. [62]

    Maltsev and M

    A. Maltsev and M. Osman. Bulk universality for complex non-Hermitian matrices with in- dependent and identically distributed entries.Probab. Theory Related Fields, 193(1):289– 334, 2025

  63. [63]

    Mandelbrot

    B. Mandelbrot. Multiplications al´ eatoires it´ er´ ees et distributions invariantes par moyenne pond´ er´ ee al´ eatoire.CR Acad. Sci. Paris, 278(289-292):355–358, 1974

  64. [64]

    B. B. Mandelbrot. Intermittent turbulence in self-similar cascades: divergence of high moments and dimension of the carrier.J. Fluid Mech., 62(2):331–358, 1974

  65. [65]

    Miller and S

    J. Miller and S. Sheffield. Liouville quantum gravity and the Brownian map I: the QLE p8{3,0qmetric.Invent. Math., 219(1):75–152, 2020

  66. [66]

    Nikula, E

    M. Nikula, E. Saksman, and C. Webb. Multiplicative chaos and the characteristic poly- nomial of the CUE: TheL 1–phase.Trans. Am. Math. Soc., 373(6):3905–3965, 2020

  67. [67]

    A. M. Obukhov. Some specific features of atmospheric turbulence.J. Geophys. Res., 67(8):3011–3014, 1962

  68. [68]

    M. Osman. Bulk universality for real matrices with independent and identically dis- tributed entries.Electron. J. Probability, 30:1–66, 2025

  69. [69]

    Rhodes and V

    R. Rhodes and V. Vargas. Two decades of probabilistic approach to liouville conformal field theory.Proceedings of the ICM 2026, 2025

  70. [70]

    Rider and B

    B. Rider and B. Vir´ ag. The noise in the circular law and the Gaussian free field.Int. Math. Res. Not., 2007:rnm006, 2007

  71. [71]

    Serebryakov and N

    A. Serebryakov and N. Simm. Schur function expansion in non-hermitian ensembles and averages of characteristic polynomials.Ann. Henri Poincar´ e, 26(6):1927–1974, 2025

  72. [72]

    Sheffield

    S. Sheffield. What is a random surface? InInternational Congress of Mathematicians, pages 1202–1258. European Mathematical Society-EMS-Publishing House GmbH, 2023

  73. [73]

    Tao and V

    T. Tao and V. Vu. Random matrices: The distribution of the smallest singular values. Geom. Func. Anal., 20(1):260–297, 2010

  74. [74]

    Tao and V

    T. Tao and V. Vu. Random matrices: universality of local eigenvalue statistics.Acta Math., 206:127–204, 2011

  75. [75]

    T. Tao, V. Vu, and M. Krishnapur. Random matrices: Universality of ESDs and the circular law.Ann. Probab., 38(5):2023–2065, 2010

  76. [76]

    A. Voros. Spectral functions, special functions and the Selberg zeta function.Comm. Math. Phys., 110(3):439–465, 1987

  77. [77]

    C. Webb. The characteristic polynomial of a random unitary matrix and Gaussian mul- tiplicative chaos—theL 2–phase.Electron. J. Probab, 20(104):21, 2015

  78. [78]

    Webb and M

    C. Webb and M. D. Wong. On the moments of the characteristic polynomial of a Ginibre random matrix.Proc. Lond. Math. Soc., 118(5):1017–1056, 2019. 80