pith. machine review for the scientific record. sign in

arxiv: 2604.12141 · v2 · submitted 2026-04-13 · 🪐 quant-ph · math-ph· math.MP

Recognition: unknown

Quantum chaotic systems: a random-matrix approach

Authors on Pith no claims yet

Pith reviewed 2026-05-10 15:01 UTC · model grok-4.3

classification 🪐 quant-ph math-phmath.MP
keywords random matrix theoryquantum chaoseigenvalue statisticssymmetry classificationunfolding procedurecorrelation functionsDyson's threefold wayAltland-Zirnbauer tenfold way
0
0 comments X

The pith

To apply random matrix theory correctly to quantum chaotic systems, the spectrum must be prepared by unfolding and the ensemble identified by symmetry class before comparison.

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

The paper reviews the steps needed to compare random matrix predictions with actual quantum energy levels. First the spectrum is unfolded by dividing out the local average spacing so that statistics are position-independent. Then the Hamiltonian's symmetries determine which of the ten possible ensembles applies, fixing the form of all correlation functions. This matters because it turns the study of chaotic quantum systems into a problem of identifying the right symmetry class rather than solving the dynamics in detail. The methods include joint eigenvalue densities, orthogonal polynomials, and links to nonlinear sigma models.

Core claim

Proper preparation of the spectrum through unfolding and correct identification of the random matrix ensemble from symmetry classification yields Dyson's threefold and Altland-Zirnbauer's tenfold way, from which joint probability densities and k-point correlation functions follow, along with relations to effective Lagrangians.

What carries the argument

Symmetry classification of matrix spaces yielding the tenfold way, combined with the unfolding procedure using the local mean level spacing to obtain universal local statistics.

Load-bearing premise

The symmetry classifications and unfolding procedures cover all relevant quantum chaotic systems without unaccounted system-specific effects.

What would settle it

A quantum system with prepared spectrum whose k-point correlations deviate from all tenfold-way predictions for its symmetry class would contradict the claims.

Figures

Figures reproduced from arXiv: 2604.12141 by Mario Kieburg.

Figure 6
Figure 6. Figure 6: Starting from this quantity, we may compute the number variance, given by (76) with [PITH_FULL_IMAGE:figures/full_fig_p021_6.png] view at source ↗
read the original abstract

We review the ideas of how random matrix theory has to be properly applied to quantum physics; particularly we focus on how the spectrum has to be properly prepared and the random matrix correctly identified before the random matrix and the physical eigenvalue spectrum can be compared. We explain the ideas of the symmetry classification of symmetric matrix spaces and how that yields Dyson's threefold and Altland-Zirnbauer's tenfold way. We also outline how the joint probability density function of the eigenvalues can be calculated from a given probability density function on the matrix space. Furthermore, we dive into the subtleties of the unfolding procedure. For this purpose, we explain the ideas of the local mean level spacing, the local level spacing distribution and the $k$-point correlation functions. We outline the techniques of orthogonal polynomials, determinantal and Pfaffian point processes and their related Fredholm determinants and Pfaffians as well as the supersymmetry method. Moreover, we relate the local spectral statistics to effective Lagrangians that give the relation to non-linear $\sigma$-models. In all these discussions, we also make brief excursions to non-Hermitian random matrix theory which are useful when studying open quantum systems, for instance.

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 / 3 minor

Summary. The manuscript is a review that explains the proper application of random matrix theory to quantum chaotic systems. It focuses on preparing the eigenvalue spectrum and identifying the correct ensemble via symmetry classifications, which yield Dyson's threefold way and Altland-Zirnbauer's tenfold way. The paper outlines the derivation of joint eigenvalue probability densities from matrix-space measures, the unfolding procedure based on local mean level spacing, and the evaluation of k-point correlation functions using orthogonal polynomials, determinantal/Pfaffian point processes, Fredholm determinants/Pfaffians, and the supersymmetry method. It also relates local statistics to effective Lagrangians and nonlinear sigma-models, with brief excursions to non-Hermitian RMT relevant for open quantum systems.

Significance. If the explanations hold, the review would provide a consolidated pedagogical resource on standard RMT techniques for spectral statistics in quantum chaos. It emphasizes practical subtleties in ensemble identification and unfolding that are often sources of error when comparing physical data to RMT predictions. The inclusion of both Hermitian and non-Hermitian cases broadens utility. As an expository work with no new derivations or claims, its value lies in clarity and accessibility rather than novelty.

major comments (1)
  1. The central claim that the outlined symmetry classifications, unfolding, and correlation techniques constitute the standard and sufficient framework for quantum chaotic systems (as stated in the abstract) requires explicit discussion of system-specific caveats, such as additional conserved quantities, finite-size effects, or deviations in disordered or open systems; without this, the generality asserted in the review risks overstatement.
minor comments (3)
  1. Clarify the transition between the joint eigenvalue density derivation and the unfolding procedure; an explicit example equation linking the two would improve readability.
  2. Ensure consistent notation for the local mean level spacing and k-point functions across sections discussing orthogonal polynomials and supersymmetry.
  3. Add a short concluding section summarizing practical steps for applying the methods to a new physical spectrum, to reinforce the review's applied focus.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive recommendation for minor revision. The feedback is appreciated as it helps ensure the review accurately reflects the scope and limitations of the RMT framework. We address the major comment below.

read point-by-point responses
  1. Referee: The central claim that the outlined symmetry classifications, unfolding, and correlation techniques constitute the standard and sufficient framework for quantum chaotic systems (as stated in the abstract) requires explicit discussion of system-specific caveats, such as additional conserved quantities, finite-size effects, or deviations in disordered or open systems; without this, the generality asserted in the review risks overstatement.

    Authors: We appreciate the referee's observation regarding the need for balance in presenting the framework. The manuscript is structured as a focused review on the standard procedures for symmetry classification (Dyson's threefold and Altland-Zirnbauer's tenfold ways), spectrum unfolding, and correlation function evaluation, with the abstract emphasizing proper preparation of the eigenvalue spectrum and correct ensemble identification prior to comparison. While these techniques form the core of the standard approach in the literature, we agree that an explicit discussion of applicability limits would strengthen the presentation and mitigate any risk of overgeneralization. In the revised version, we will add a concise subsection (positioned after the introduction or in a new 'Scope and Limitations' section) that outlines key caveats, including: (i) additional conserved quantities that may induce block-diagonal structures requiring separate unfolding per block; (ii) finite-size effects in small systems where universal statistics emerge only asymptotically; and (iii) deviations in disordered or open systems, where the brief non-Hermitian excursions already present in the text can be expanded to note modifications to the sigma-model or correlation functions. This addition will be kept brief to preserve the pedagogical focus while clarifying the framework's domain of validity. revision: yes

Circularity Check

0 steps flagged

Review paper restating standard RMT results with no novel derivations

full rationale

This is an expository review summarizing established random matrix theory techniques for quantum spectra, including Dyson's threefold and Altland-Zirnbauer's tenfold classifications, joint eigenvalue densities via orthogonal polynomials or supersymmetry, unfolding via local mean spacing, and k-point correlations via Fredholm/Pfaffian determinants. No new theorems, predictions, or first-principles derivations are advanced; the content is restatement of prior, externally validated results. No steps reduce by construction to fitted inputs, self-definitions, or self-citation chains that bear the central claims. All referenced techniques are standard and independently checkable outside this manuscript.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The review relies entirely on established prior literature in random matrix theory and quantum mechanics; no new free parameters, ad-hoc axioms, or invented entities are introduced.

axioms (2)
  • standard math Standard results on orthogonal polynomials, determinantal point processes, and Fredholm determinants
    Invoked to obtain joint eigenvalue densities and k-point correlation functions.
  • domain assumption Symmetry classification of Hermitian and non-Hermitian matrix spaces (Dyson threefold way, Altland-Zirnbauer tenfold way)
    Taken as the basis for identifying the correct random-matrix ensemble for a given quantum system.

pith-pipeline@v0.9.0 · 5501 in / 1270 out tokens · 61875 ms · 2026-05-10T15:01:13.685636+00:00 · methodology

discussion (0)

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

Forward citations

Cited by 1 Pith paper

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

  1. Quantum graph models of quantum chaos: an introduction and some recent applications

    quant-ph 2026-04 unverdicted novelty 1.0

    Quantum graphs are presented as a paradigmatic model for quantum chaos, with the paper providing a didactical overview of foundational results and some recent developments.

Reference graph

Works this paper leans on

204 extracted references · 147 canonical work pages · cited by 1 Pith paper · 8 internal anchors

  1. [1]

    Wishart,The generalised product moment distribution in samples from a normal multivariate population,Biometrika10(1982) 32–52

    J. Wishart,The generalised product moment distribution in samples from a normal multivariate population,Biometrika10(1982) 32–52

  2. [2]

    Paul and A

    D. Paul and A. Aue,Random matrix theory in statistics: A review,J. Stat. Plan. Inference150(2014) 1–29

  3. [3]

    Mar ˇcenko and L.A

    V.A. Mar ˇcenko and L.A. Pastur,Distribution of eigenvalues for some sets of random matrices,Math. USSR Sb.1(1967) 457–483

  4. [4]

    Romain, S

    C. Romain, S. Antipolis and M. Debbah,Random Matrix Methods for Wireless Communications, Cambridge University Press, 1st ed. (2011)

  5. [5]

    Wigner,Characteristic vectors of bordered matrices with infinite dimensions,Ann

    E.P . Wigner,Characteristic vectors of bordered matrices with infinite dimensions,Ann. Math.62(1955) 548–564

  6. [6]

    Wigner,Results and theory of resonance absorbtion,Conference on Neutron Physics by Time-of-Flight, Gatlinburg, Tennessee (1956) 59–70

    E.P . Wigner,Results and theory of resonance absorbtion,Conference on Neutron Physics by Time-of-Flight, Gatlinburg, Tennessee (1956) 59–70

  7. [7]

    Tao and V

    T. Tao and V. Vu,Random matrices: Localization of the eigenvalues and the necessity of four moments,Acta Math. Vietnam.36(2011) 431–449 [arXiv:1005.2901]

  8. [8]

    Grobe, F

    R. Grobe, F . Haake and H.-J. Sommers,Quantum distinction of regular and chaotic dissipative motion,Phys. Rev. Lett.61(1988) 1899–1902

  9. [9]

    Hua,Harmonic analysis of functions of several complex variables in the classical domains, American Mathematical Society, 1st ed

    L.K. Hua,Harmonic analysis of functions of several complex variables in the classical domains, American Mathematical Society, 1st ed. (1963)

  10. [10]

    S. Helgason,Groups and Geometric Analysis: Integral Geometry, Invariant Differential Operators and Spherical Functions, Mathematical Survey and Monographs83, American Mathematical Society, 1st ed. (2000)

  11. [11]

    Diaconis and P .J

    P . Diaconis and P .J. Forrester,A. hurwitz and the origins of random matrix theory in mathematics,Random Matrices Theory Appl.06 (2017) 1730001 [arXiv:1512.09229]

  12. [12]

    Hurwitz,Ueber die erzeugung der invarianten durch integration,Nachr

    A. Hurwitz,Ueber die erzeugung der invarianten durch integration,Nachr. Ges. Wiss. G ¨ottingen1897(1897) 71–90

  13. [13]

    Euler,Problema algebraicum ob affectiones prorsus singulares,Opera omnia 1st series6(1770) 287–315

    L. Euler,Problema algebraicum ob affectiones prorsus singulares,Opera omnia 1st series6(1770) 287–315

  14. [14]

    Harish-Chandra,Invariant differential operators on a semisimple Lie algebra,Proc. Natl. Acad. Sci. USA42(1956) 252–253

  15. [15]

    Itzykson and J.B

    C. Itzykson and J.B. Zuber,The planar approximation II,J. Math. Phys.21(1980) 411–421

  16. [16]

    Bohigas, M.J

    O. Bohigas, M.J. Giannoni and C. Schmit,Characterization of chaotic quantum syectra and universality of level fluctuation laws,Phys. Rev. Lett.52(1984) 1–4

  17. [17]

    Berry and M

    M.V. Berry and M. Tabor,Level clustering in the regular spectrum,Proc. R. Soc. Lond. Ser. A Math. Phys. Sci.356(1977) 375–394

  18. [18]

    Braun and F

    P . Braun and F . Haake,Level statistics in arithmetical and pseudo-arithmetical chaos,J. Phys. A43(2010) 262001 [arXiv:1001.3339]

  19. [19]

    Kubo,Electronic properties of metallic fine particles

    R. Kubo,Electronic properties of metallic fine particles. I.,J. Phys. Soc. Jpn.17(1962) 975–986

  20. [20]

    Gor’kov and G.M

    L.P . Gor’kov and G.M. Eliashberg,Minute metallic particles in an electromagnetic field,J. Exp. Theor. Phys.21(1965) 940–947

  21. [21]

    Beenakker,Random-matrix theory of Majorana fermions and topological superconductors,Rev

    C.W.J. Beenakker,Random-matrix theory of Majorana fermions and topological superconductors,Rev. Mod. Phys.87(2015) 1037–1066 [arXiv:1407.2131]

  22. [22]

    Beenakker,Condensed matter physics, Chapter 35 in [206], Oxford University Press (2011) [arXiv:0904.1432]

    C.W.J. Beenakker,Condensed matter physics, Chapter 35 in [206], Oxford University Press (2011) [arXiv:0904.1432]

  23. [23]

    Anderson,Absence of diffusion in certain random lattices,Phys

    P .W. Anderson,Absence of diffusion in certain random lattices,Phys. Rev.109(1958) 1492–1505

  24. [24]

    Bourgade,Random band matrices, inProceedings of the International Congress of Mathematicians (ICM 2018), p

    P . Bourgade,Random band matrices, inProceedings of the International Congress of Mathematicians (ICM 2018), p. 2759–2783 (2019) [arXiv:1807.03031]

  25. [25]

    The spectrum of the QCD Dirac operator and chiral random matrix theory: the threefold way

    J.J.M. Verbaarschot,The spectrum of the QCD dirac operator and chiral random matrix theory: the threefold way,Phys. Rev. Lett.72 (1994) 2531–2533 [arXiv:hep-th/9401059]

  26. [26]

    Stephanov,Dirac operator as a random matrix and the quenched limit of QCD with chemical potential,Nucl

    M.A. Stephanov,Dirac operator as a random matrix and the quenched limit of QCD with chemical potential,Nucl. Phys. Proc. Suppl.53 (1997) 469–471 [arXiv:hep-lat/9607060]

  27. [28]

    Damgaard, K

    P .H. Damgaard, K. Splittorff and J.J.M. Verbaarschot,Microscopic spectrum of the Wilson Dirac operator,Phys. Rev. Lett.105(2010) 162002 [arXiv:1001.2937]

  28. [30]

    Kieburg, J.J.M

    M. Kieburg, J.J.M. Verbaarschot and T. Wettig,Dirac spectrum and chiral condensate for QCD at fixedθ-angle,Phys. Rev. D99(2019) 074515 [arXiv:1809.09773]

  29. [31]

    Collins and I

    B. Collins and I. Nechita,Random matrix techniques in quantum information theory,J. Math. Phys.57(2016) 015215 [arXiv:1509.04689]

  30. [32]

    Quantum Chaos and Quantum Information: Interactions and Implications

    A. Lakshminarayan and K. ˙Zyczkowski,Quantum chaos and quantum information: Interactions and implications, chapter in quantum chaos volume in “comprehensive quantum mechanics”, (2026) [arXiv:2604.12267]

  31. [33]

    Lloyd and H

    S. Lloyd and H. Pagels,Complexity as thermodynamic depth,Ann. Phys.188(1988) 186–213

  32. [34]

    Average Entropy of a Subsystem

    D.N. Page,Average entropy of a subsystem,Phys. Rev. Lett.71(1993) 1291–1294 [arXiv:gr-qc/9305007]

  33. [35]

    ˙Zyczkowski, K.A

    K. ˙Zyczkowski, K.A. Penson, I. Nechita and B. Collins,Generating random density matrices,J. Math. Phys.52(2011) 062201 [arXiv:1010.3570]

  34. [36]

    Lubkin,Entropy of an n-system from its correlation with ak-reservoir,J

    E. Lubkin,Entropy of an n-system from its correlation with ak-reservoir,J. Math. Phys.19(1978) 1028–1031

  35. [37]

    Bruzda, V

    W. Bruzda, V. Cappellini, H.-J. Sommers and K. ˙Zyczkowski,Random quantum operations,Phys. Lett. A373(2009) 320–324 [arXiv:0804.2361]

  36. [38]

    Akemann, M

    G. Akemann, M. Kieburg and L. Wei,Singular value correlation functions for products of Wishart random matrices,J. Phys. A46(2013) 275205 [arXiv:1303.5694]. 32Quantum chaotic systems: a random-matrix approach

  37. [39]

    Dorokhov,Transmission coefficient and the localization length of an electron inNbound disordered chains,JETP Lett.36(1982) 318–321

    O.N. Dorokhov,Transmission coefficient and the localization length of an electron inNbound disordered chains,JETP Lett.36(1982) 318–321

  38. [40]

    Mello, P

    P .A. Mello, P . Pereyra and N. N. Kumar,Macroscopic approach to multichannel disordered conductors,Ann. Phys. (N.Y)181(1988) 290–317

  39. [41]

    Ipsen and H

    J.R. Ipsen and H. Schomerus,Isotropic brownian motions over complex fields as a solvable model for May-Wigner stability analysis,J. Phys. A49(2016) 385201 [arXiv:1602.06364]

  40. [42]

    2D Gravity and Random Matrices

    P . Di Francesco, P . Ginsparg and J. Zinn-Justin,2D gravity and random matrices,Phys. Rept.254(1995) 1–133 [arXiv:hep-th/9306153]

  41. [43]

    Gurau and V

    R. Gurau and V. Rivasseau,Quantum gravity and random tensors,arXiv:2401.13510

  42. [44]

    Liouville quantum gravity from random matrix dynamics.arXiv preprint arXiv:2206.03029(2022)

    P . Bourgade and H. Falconet,Liouville quantum gravity from random matrix dynamics,arXiv:2206.03029

  43. [45]

    Eynard and N

    B. Eynard and N. Orantin,Topological recursion in enumerative geometry and random matrices,J. Phys. A42(2009) 293001 [arXiv:0811.3531]

  44. [46]

    Kota,Embedded Random Matrix Ensembles in Quantum Physics, Springer, 1st ed

    V.K.B. Kota,Embedded Random Matrix Ensembles in Quantum Physics, Springer, 1st ed. (2014)

  45. [47]

    Lueck, H.-J

    T. Lueck, H.-J. Sommers and M.R. Zirnbauer,Energy correlations for a random matrix model of disordered bosons,J. Math. Phys.47 (2006) 103304 [arXiv:cond-mat/0607243]

  46. [48]

    Bianchi, L

    E. Bianchi, L. Hackl, M. Kieburg, M. Rigol and L. Vidmar,Volume-law entanglement entropy of typical pure quantum states,Phys. Rev. X 3(2022) 030201 [arXiv:2112.06959]

  47. [49]

    Aurell, L

    E. Aurell, L. Hackl, P . Horodecki, R.H. Jonsson and M. Kieburg,Random pure gaussian states and Hawking radiation,Phys. Rev. Lett. 133(2024) 060202 [arXiv:2311.10562]

  48. [50]

    Gapless Spin-Fluid Ground State in a Random Quantum Heisenberg Magnet

    S. Sachdev and J. Y e,Gapless spin-fluid ground state in a random quantum Heisenberg magnet,Phys. Rev. Lett.70(1993) 3339–3342 [arXiv:cond-mat/9212030]

  49. [51]

    Kumar, A

    S. Kumar, A. Nock, H.-J. Sommers, T. Guhr, B. Dietz, M. Miski-Oglu et al.,Distribution of scattering matrix elements in quantum chaotic scattering,Phys. Rev. Lett.111(2013) 030403 [arXiv:1304.5284]

  50. [52]

    Schomerus,Random matrix approaches to open quantum systems, inStochastic Processes and Random Matrices: Lecture Notes of the Les Houches Summer School, July 2015, vol

    H. Schomerus,Random matrix approaches to open quantum systems, inStochastic Processes and Random Matrices: Lecture Notes of the Les Houches Summer School, July 2015, vol. 104, p. 409–473, Oxford University Press (2017) [arXiv:1610.05816]

  51. [53]

    Fyodorov and D.V

    Y .V. Fyodorov and D.V. Savin,Resonance scattering of waves in chaotic systems, Chapter 34 in [206], Oxford University Press (2011)

  52. [54]

    Abul-Magd and A.Y

    A.A. Abul-Magd and A.Y . Abul-Magd,Unfolding of the spectrum for chaotic and mixed systems,Physica A396(2014) 185–194 [arXiv:1311.2419]

  53. [55]

    Schnyder, S

    A.P . Schnyder, S. Ryu, A. Furusaki and A.W.W. Ludwig,Classification of topological insulators and superconductors in three spatial dimensions,Phys. Rev. B78(2008) 195125 [arXiv:0803.2786]

  54. [56]

    DeJonghe, K

    R. DeJonghe, K. Frey and T. Imbo,Bott periodicity and realizations of chiral symmetry in arbitrary dimensions,Phys. Lett B718(2012) 603–609 [arXiv:1207.6547]

  55. [57]

    Kieburg and T.R

    M. Kieburg and T.R. W ¨urfel,Global symmetries of naive and staggered Fermions in arbitrary dimensions,Phys. Rev. D96(2017) 034502 [arXiv:1710.03049]

  56. [58]

    Complete random matrix classification of SYK models with N= 0, 1 and 2 supersymmetry,

    T. Kanazawa and T. Wettig,Complete random matrix classification of SYK models withN=0,1and2supersymmetry,J. High Energ. Phys.09(2017) 050 [arXiv:1706.03044]

  57. [59]

    Verbaarschot,Quantum chromodynamics, Chapter 32 in [206], Oxford University Press (2011) [arXiv:0910.4134]

    J.J.M. Verbaarschot,Quantum chromodynamics, Chapter 32 in [206], Oxford University Press (2011) [arXiv:0910.4134]

  58. [60]

    Efetov,Supersymmetry in Disorder and Chaos, Cambridge University Press, 1st ed

    K. Efetov,Supersymmetry in Disorder and Chaos, Cambridge University Press, 1st ed. (1996)

  59. [61]

    Sommers, Y .V

    H.-J. Sommers, Y .V. Fyodorov and M. Titov,S-matrix poles for chaotic quantum systems as eigenvalues of complex symmetric random matrices: from isolated to overlapping resonances,J. Phys. A32(1999) L77 [arXiv:chao-dyn/9807015]

  60. [62]

    Kieburg, J.J.M

    M. Kieburg, J.J.M. Verbaarschot and S. Zafeiropoulos,Spectral properties of the Wilson Dirac operator and random matrix theory,Phys. Rev. D88(2013) 094502 [arXiv:1307.7251]

  61. [63]

    Nowak and W

    M.A. Nowak and W. Tarnowski,Spectra of large time-lagged correlation matrices from random matrix theory,J. Stat. Mech.2017(2017) 063405 [arXiv:1612.06552]

  62. [64]

    Wigner,Normal form of antiunitary operators,J

    E.P . Wigner,Normal form of antiunitary operators,J. Math. Phys.1(1960) 409–413

  63. [65]

    Dyson,The threefold way

    F .J. Dyson,The threefold way. Algebraic structure of symmetry groups and ensembles in quantum mechanics,J. Math. Phys.3(1962) 1199–1215

  64. [66]

    Altland and M.R

    A. Altland and M.R. Zirnbauer,Novel symmetry classes in mesoscopic normal-superconducting hybrid structures,Phys. Rev. B55 (1997) 1142–1161 [arXiv:cond-mat/9602137]

  65. [67]

    Forrester,Log-Gases and Random Matrices, Princeton University Press, 1st ed

    P .J. Forrester,Log-Gases and Random Matrices, Princeton University Press, 1st ed. (2010)

  66. [68]

    Dietz and F

    B. Dietz and F . Haake,Taylor and Pad ´e analysis of the level spacing distributions of random-matrix ensembles,Z. Phys. B Condensed Matter80(1990) 153–158

  67. [69]

    Dumitriu and A

    I. Dumitriu and A. Edelman,Matrix models for beta ensembles,J. Math. Phys.43(2002) 5830–5847 [arXiv:math-ph/0206043]

  68. [70]

    Ivanov,The supersymmetric technique for random-matrix ensembles with zero eigenvalues,J

    D.A. Ivanov,The supersymmetric technique for random-matrix ensembles with zero eigenvalues,J. Math. Phys.43,(2002) 126–153 [arXiv:cond-mat/0103137]

  69. [71]

    Helgason,Differential Geometry, Lie Groups, and Symmetric Spaces, Academic Press, 1st ed

    S. Helgason,Differential Geometry, Lie Groups, and Symmetric Spaces, Academic Press, 1st ed. (1978)

  70. [72]

    Bruckmann, S

    F . Bruckmann, S. Keppeler, M. Panero and T. Wettig,Polyakov loops and spectral properties of the staggered Dirac operator,Phys. Rev. D78(2008) 034503 [arXiv:0804.3929]

  71. [73]

    Osborn,Staggered chiral random matrix theory,Phys

    J.C. Osborn,Staggered chiral random matrix theory,Phys. Rev. D83(2011) 034505 [arXiv:1012.4837]

  72. [74]

    Anderson,Spectral statistics of unitary ensembles, Chapter 4 in [206], Oxford University Press (2011)

    G.W. Anderson,Spectral statistics of unitary ensembles, Chapter 4 in [206], Oxford University Press (2011)

  73. [75]

    Andr ´eief,Notes sur une relation les int ´egrales d´efinies des produits des fonctions,M ´em

    K.A. Andr ´eief,Notes sur une relation les int ´egrales d´efinies des produits des fonctions,M ´em. de la Soc. Sci., Bordeaux2(1886) 1–14

  74. [76]

    Bernard and A

    D. Bernard and A. LeClair,A classification of non-Hermitian random matrices, inCappelli, A., Mussardo, G. (eds) Statistical Field Theories. NATO Science Series, 73, Springer, 2002 [arXiv:cond-mat/0110649]

  75. [77]

    Magnea,Random matrices beyond the Cartan classification,J

    U. Magnea,Random matrices beyond the Cartan classification,J. Phys. A41(2008) 045203 [arXiv:0707.0418]

  76. [78]

    Kawabata, K

    K. Kawabata, K. Shiozaki, M. Ueda and M. Sato,Symmetry and topology in non-Hermitian physics,Phys. Rev. X9(2019) 041015 [arXiv:1812.09133]

  77. [79]

    Garc ´ıa-Garc´ıa, L

    A.M. Garc ´ıa-Garc´ıa, L. S´a and J.J.M. Verbaarschot,Symmetry classification and universality in non-Hermitian many-body quantum chaos by the Sachdev-Ye-Kitaev model,Phys. Rev. X12(2022) 021040 [arXiv:2110.03444]

  78. [80]

    L. S ´a, P . Ribeiro and T. Prosen,Symmetry classification of many-body Lindbladians: Tenfold way and beyond,Phys. Rev. X13(2023) 031019 [arXiv:2212.00474]

  79. [81]

    L. S ´a, P . Ribeiro, T. Prosen and D. Bernard,Symmetry classes of classical stochastic processes,J. Stat. Phys.192(2025) 41 [arXiv:2406.17955]

  80. [82]

    Ginibre,Statistical ensembles of complex, quaternion, and real matrices,J

    J. Ginibre,Statistical ensembles of complex, quaternion, and real matrices,J. Math. Phys.6(1965) 440–449. Quantum chaotic systems: a random-matrix approach33

Showing first 80 references.