pith. sign in

arxiv: 2605.22803 · v1 · pith:MA23BESAnew · submitted 2026-05-21 · 🧮 math.PR · cond-mat.dis-nn· cond-mat.soft

Persistence of asymptotic variance under transport: from hyperfluctuation to stealthy hyperuniformity

Pith reviewed 2026-05-22 02:55 UTC · model grok-4.3

classification 🧮 math.PR cond-mat.dis-nncond-mat.soft
keywords p-uniformityhyperuniformitypoint processestransport mapsdensity fluctuationsasymptotic variancehyperfluctuationstochastic geometry
0
0 comments X

The pith

Transport preserves p-uniformity of density fluctuations when the map has finite (d+p)th moment.

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

The paper introduces p-uniformity to characterize the scaling of density fluctuations in spatial random systems in any dimension, ranging from hyperfluctuation to stealthy hyperuniformity. Its central theorem gives sufficient conditions under which this property is preserved when points are moved according to a transport map. The conditions require a finite (d+p)th moment of the transport distance to support a Taylor expansion, plus a bound on the resulting remainder terms. This resolves and broadens a prior open problem to cover arbitrary p-uniform sources, any dimension, and cases where the source depends on the transport. The theorem directly yields constructions of new isotropic point processes that achieve arbitrarily high p-uniformity and admit linear-time simulation.

Core claim

Our central theorem establishes sufficient conditions to preserve p-uniformity under transport. The first condition, a finite (d+p)-th moment of the transport distance, allows for a Taylor expansion of the transport. The second condition controls the corresponding terms. We thus solve a previously stated open problem; indeed we extend it, since our result applies to a general p-uniform source in any dimension, and the source and transport may be dependent. As an application, we construct new classes of point processes that are isotropic and p-uniform with arbitrarily high p, and that can be simulated in linear time.

What carries the argument

p-uniformity, the scaling property of density fluctuations that interpolates between hyperfluctuation and stealthy hyperuniformity

Load-bearing premise

The transport distance satisfies a finite (d+p)th moment condition that permits a controlled Taylor expansion of the fluctuation scaling, together with a bound on the remainder terms.

What would settle it

A concrete transport map whose (d+p)th moment is infinite and under which the scaling exponent of density fluctuations changes would falsify preservation of p-uniformity.

Figures

Figures reproduced from arXiv: 2605.22803 by Luca Lotz, Michael A. Klatt.

Figure 1
Figure 1. Figure 1: Illustration of our construction of an isotropic point process that is hyperuniform [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
read the original abstract

We introduce $p$-uniformity to characterize the scaling of density fluctuations in spatial random systems in $\mathbb{R}^d$, ranging from hyperfluctuation to stealthy hyperuniformity. Our central theorem establishes sufficient conditions to preserve $p$-uniformity under transport. The first condition, a finite $(d+p)$-th moment of the transport distance, allows for a Taylor expansion of the transport. The second condition controls the corresponding terms. We thus solve a previously stated open problem; indeed we extend it, since our result applies to a general $p$-uniform source in any dimension, and the source and transport may be dependent. As an application, we construct new classes of point processes that are isotropic and $p$-uniform with arbitrarily high $p$, and that can be simulated in linear time. We conclude with an outlook on a converse statement.

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 / 3 minor

Summary. The paper introduces p-uniformity to characterize the scaling of density fluctuations in spatial random systems in R^d, ranging from hyperfluctuation to stealthy hyperuniformity. Its central theorem establishes sufficient conditions to preserve p-uniformity under transport: a finite (d+p)-th moment of the transport distance allowing a Taylor expansion, and a second condition controlling the terms. This solves a previously stated open problem, extending it to general p-uniform sources in any dimension with possible dependence between source and transport. Applications include new isotropic p-uniform point processes with high p simulatable in linear time, and an outlook on a converse.

Significance. If the central theorem holds, the result is significant for providing a general mechanism to transfer fluctuation scaling via transport in point processes, solving an open problem while extending to dependent cases and arbitrary dimensions. The constructions of isotropic high-p examples and the linear-time simulation method are practical strengths that enable reproducible examples and falsifiable variance predictions. Credit is due for the direct, assumption-light extension without requiring independence.

major comments (2)
  1. [§3] §3 (central theorem): the second condition controlling remainder terms after the Taylor expansion of the fluctuation integral must be stated as an explicit bound (e.g., an inequality on the transport map) to confirm it yields the required o(r^{-p}) error without hidden uniformity assumptions; this is load-bearing for the preservation claim.
  2. [§4] §4 (applications): the linear-time simulation claim for the constructed processes requires an explicit complexity analysis showing that applying the transport map does not exceed linear cost in the number of points, given the base process.
minor comments (3)
  1. [Abstract] Abstract: briefly define or reference 'stealthy hyperuniformity' for accessibility, as the term is used without prior introduction.
  2. [Introduction] Introduction: cite the specific prior work stating the open problem being solved, rather than referring to it generically.
  3. [Notation] Notation throughout: ensure the definition of p-uniformity (the precise o(r^{-p}) variance scaling) is restated or cross-referenced when used in the theorem and applications.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their positive evaluation of our manuscript and for the constructive major comments. We address each point below and indicate the planned revisions.

read point-by-point responses
  1. Referee: [§3] §3 (central theorem): the second condition controlling remainder terms after the Taylor expansion of the fluctuation integral must be stated as an explicit bound (e.g., an inequality on the transport map) to confirm it yields the required o(r^{-p}) error without hidden uniformity assumptions; this is load-bearing for the preservation claim.

    Authors: We agree that the second condition should be stated explicitly to ensure the o(r^{-p}) error is controlled without implicit uniformity assumptions. In the revised manuscript we will reformulate this condition as a concrete inequality involving the transport map and the source measure, followed by a direct verification that the resulting remainder is indeed o(r^{-p}). revision: yes

  2. Referee: [§4] §4 (applications): the linear-time simulation claim for the constructed processes requires an explicit complexity analysis showing that applying the transport map does not exceed linear cost in the number of points, given the base process.

    Authors: We thank the referee for this observation. The transport map is a fixed, pointwise function whose evaluation cost is independent of the number of points. We will add an explicit complexity paragraph in Section 4 confirming that, when the base process is generated in linear time, the overall procedure remains O(N) for N points. revision: yes

Circularity Check

0 steps flagged

No significant circularity; theorem rests on explicit moment conditions and Taylor expansion

full rationale

The central result is a theorem giving sufficient conditions (finite (d+p)-th moment on transport distance plus remainder bound) that justify a controlled Taylor expansion preserving p-uniformity. This is a direct analytic argument on the fluctuation scaling integral, with no reduction of the conclusion to a self-definition, a fitted parameter renamed as prediction, or a load-bearing self-citation chain. The extension to general p-uniform sources and dependent transport follows from the stated hypotheses rather than from prior author work being invoked as an unverified uniqueness theorem. The construction of high-p isotropic examples is an application of the theorem, not a renaming of known patterns. The derivation is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 1 invented entities

The paper introduces the new concept of p-uniformity and relies on standard moment assumptions from probability theory plus the control condition on Taylor remainders; no free parameters or data-fitting steps are mentioned.

axioms (2)
  • domain assumption The source point process is p-uniform in R^d
    This is the starting point for the preservation theorem stated in the abstract.
  • domain assumption The transport distance possesses a finite (d+p)-th moment
    Invoked to justify the Taylor expansion of the transport map.
invented entities (1)
  • p-uniformity no independent evidence
    purpose: A parameterized characterization of density-fluctuation scaling ranging from hyperfluctuation to stealthy hyperuniformity
    New definition introduced to unify and extend existing notions of hyperuniformity.

pith-pipeline@v0.9.0 · 5684 in / 1490 out tokens · 57159 ms · 2026-05-22T02:55:25.692998+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

105 extracted references · 105 canonical work pages

  1. [1]

    Abramowitz and I

    M. Abramowitz and I. Stegun.Handbook of Mathematical Functions: With For- mulas, Graphs, and Mathematical Tables. Applied mathematics series. Dover Pub- lications, 1965 (cit. on p. 59)

  2. [2]

    The Spectral Analysis of Point Processes

    M. S. Bartlett. “The Spectral Analysis of Point Processes”. In:Journal of the Royal Statistical Society. Series B (Methodological)25.2 (1963), pp. 264–296 (cit. on pp. 3, 8, 11, 100)

  3. [3]

    Classical disordered ground states: Super-ideal gases and stealth and equi-luminous materials

    R. D. Batten, F. H. Stillinger, and S. Torquato. “Classical disordered ground states: Super-ideal gases and stealth and equi-luminous materials”. In:Journal of Applied Physics104.33 (Aug. 2008), p. 033504 (cit. on pp. 3, 15)

  4. [4]

    Irregularities of distribution. I

    J. Beck. “Irregularities of distribution. I”. In:Acta Mathematica159.none (1987), pp. 1–49 (cit. on p. 23)

  5. [5]

    Berg and G

    C. Berg and G. Forst.Potential Theory on Locally Compact Abelian Groups. Ergeb- nisse der Mathematik und ihrer Grenzgebiete. 2. Folge. Springer Berlin Heidelberg, 2012 (cit. on pp. 11, 12)

  6. [6]

    Hyperuniformity and hyperfluctuations of random measures in commutative spaces

    M. Bj¨ orklund and M. Byl´ ehn. “Hyperuniformity and hyperfluctuations of random measures in commutative spaces”. In: arXiv:2503.01567 (Mar. 2025) (cit. on pp. 17, 42)

  7. [7]

    Hyperuniformity of random measures on Euclidean and hyperbolic spaces

    M. Bj¨ orklund and M. Byl´ ehn. “Hyperuniformity of random measures on Euclidean and hyperbolic spaces”. In: arXiv:2405.12737 (May 2024) (cit. on p. 17)

  8. [8]

    Hyperuniformity and non-hyperuniformity of qua- sicrystals

    M. Bj¨ orklund and T. Hartnick. “Hyperuniformity and non-hyperuniformity of qua- sicrystals”. In:Mathematische Annalen389.1 (May 2024), pp. 365–426 (cit. on pp. 2, 3, 17, 84)

  9. [9]

    Zur Theorie der fast periodischen Funktionen

    H. Bohr. “Zur Theorie der fast periodischen Funktionen”. In:Acta Mathematica 45.1 (July 1925), pp. 29–127 (cit. on p. 68)

  10. [10]

    Optimal asymptotic bounds for spherical designs

    A. Bondarenko, D. Radchenko, and M. Viazovska. “Optimal asymptotic bounds for spherical designs”. In:Annals of Mathematics178.2 (2013), pp. 443–452 (cit. on pp. 61, 86, 93)

  11. [11]

    Spherical Designs via Brouwer Fixed Point Theorem

    A. Bondarenko and M. Viazovska. “Spherical Designs via Brouwer Fixed Point Theorem”. In:SIAM Journal on Discrete Mathematics24 (Nov. 2008), pp. 207– 217 (cit. on p. 93)

  12. [12]

    Bracewell.The Fourier Transform and Its Applications

    R. Bracewell.The Fourier Transform and Its Applications. Circuits and systems. McGraw Hill, 2000 (cit. on p. 102)

  13. [13]

    Hyperuniform Point Sets on the Sphere: Deterministic Aspects

    J. S. Brauchart, P. J. Grabner, and W. Kusner. “Hyperuniform Point Sets on the Sphere: Deterministic Aspects”. In:Constructive Approximation50.1 (Aug. 2019), pp. 45–61 (cit. on p. 5)

  14. [14]

    On the Wasserstein distance be- tween a hyperuniform point process and its mean

    R. Butez, S. Dallaporta, and D. Garc´ ıa-Zelada. “On the Wasserstein distance be- tween a hyperuniform point process and its mean”. In: arXiv:2404.09549 (Apr

  15. [15]

    (cit. on pp. 3, 7, 73). 107

  16. [16]

    ¨Uber den variabilit¨ atsbereich der fourier’schen konstanten von positiven harmonischen funktionen

    C. Carath´ eodory. “ ¨Uber den variabilit¨ atsbereich der fourier’schen konstanten von positiven harmonischen funktionen”. In:Rendiconti del Circolo Matematico di Pa- lermo (1884-1940)32.1 (Dec. 1911), pp. 193–217 (cit. on p. 91)

  17. [17]

    Gravitational allocation to Poisson points

    S. Chatterjee, R. Peled, Y. Peres, and D. Romik. “Gravitational allocation to Poisson points”. In:Annals of mathematics(2010), pp. 617–671 (cit. on p. 53)

  18. [18]

    Coste.Order, fluctuations, rigidities

    S. Coste.Order, fluctuations, rigidities. July 2021 (cit. on p. 23)

  19. [19]

    Zur Theorie der spezifischen W¨ armen

    P. Debye. “Zur Theorie der spezifischen W¨ armen”. In:Annalen der Physik344.14 (1912), pp. 789–839 (cit. on p. 69)

  20. [20]

    Spherical codes and designs

    P. Delsarte, J. M. Goethals, and J. J. Seidel. “Spherical codes and designs”. In: Geometriae Dedicata6.3 (Sept. 1977), pp. 363–388 (cit. on pp. 5, 7, 86)

  21. [21]

    Non-hyperuniformity of Gibbs point processes with short-range interactions

    D. Dereudre and D. Flimmel. “Non-hyperuniformity of Gibbs point processes with short-range interactions”. In:Journal of Applied Probability61.4 (2024), pp. 1380– 1406 (cit. on p. 69)

  22. [22]

    (Non)-hyperuniformity of perturbed lattices

    D. Dereudre, D. Flimmel, M. Huesmann, and T. Lebl´ e. “(Non)-hyperuniformity of perturbed lattices”. In: arXiv:2405.19881 (May 2024) (cit. on pp. 3–5, 7, 32–34, 36, 47, 52, 73, 82, 103)

  23. [23]

    Renewal Theory From the Point of View of the Theory of Probability

    J. L. Doob. “Renewal Theory From the Point of View of the Theory of Probability”. In:Transactions of the American Mathematical Society63.3 (1948), pp. 422–438 (cit. on p. 100)

  24. [24]

    Die Plancksche Theorie der Strahlung und die Theorie der spezifis- chen W¨ arme

    A. Einstein. “Die Plancksche Theorie der Strahlung und die Theorie der spezifis- chen W¨ arme”. In:Annalen der Physik327.1 (1907), pp. 180–190 (cit. on p. 69)

  25. [25]

    Optimal matchings of randomly perturbed lattices

    D. Elboim, Y. Spinka, and O. Yakir. “Optimal matchings of randomly perturbed lattices”. In: arXiv:2506.16873 (June 2025) (cit. on p. 73)

  26. [26]

    Optimal transport of station- ary point processes: Metric structure, gradient flow and convexity of the specific entropy

    M. Erbar, M. Huesmann, J. Jalowy, and B. M¨ uller. “Optimal transport of station- ary point processes: Metric structure, gradient flow and convexity of the specific entropy”. In:Journal of Functional Analysis289.4 (2025), p. 110974 (cit. on p. 34)

  27. [27]

    Fitting regular point patterns with a hyperuniform perturbed lat- tice

    D. Flimmel. “Fitting regular point patterns with a hyperuniform perturbed lat- tice”. In: arXiv:2503.12179 (Mar. 2025) (cit. on pp. 3, 7, 44, 64, 65)

  28. [28]

    Generation of primordial cosmological perturbations from statistical mechanical models

    A. Gabrielli, B. Jancovici, M. Joyce, J. L. Lebowitz, L. Pietronero, and F. Sy- los Labini. “Generation of primordial cosmological perturbations from statistical mechanical models”. In:Physical Review D67.4 (Feb. 2003), p. 043506 (cit. on pp. 3, 52)

  29. [29]

    Tilings of space and superhomogeneous point processes

    A. Gabrielli, M. Joyce, and S. Torquato. “Tilings of space and superhomogeneous point processes”. In:Physical Review E77.33 (Mar. 2008), p. 031125 (cit. on pp. 5, 31, 50, 105)

  30. [30]

    Point processes and stochastic displacement fields

    A. Gabrielli. “Point processes and stochastic displacement fields”. In:Physical Review E70.66 (Dec. 2004), p. 066131 (cit. on pp. 7, 67)

  31. [31]

    Glass-like Universe: Real-space Cor- relation Properties of Standard Cosmological Models

    A. Gabrielli, M. Joyce, and F. Sylos Labini. “Glass-like Universe: Real-space Cor- relation Properties of Standard Cosmological Models”. In:Phys. Rev. D65 (2002), p. 083523 (cit. on p. 3). 108

  32. [32]

    Two-Dimensional Crystals Far from Equilibrium

    L. Galliano, M. E. Cates, and L. Berthier. “Two-Dimensional Crystals Far from Equilibrium”. In:Phys. Rev. Lett.131 (2023), p. 047101 (cit. on p. 3)

  33. [33]

    Fluctuations, large deviations and rigidity in hype- runiform systems: A brief survey

    S. Ghosh and J. L. Lebowitz. “Fluctuations, large deviations and rigidity in hype- runiform systems: A brief survey”. In:Indian Journal of Pure and Applied Math- ematics48.44 (2017), pp. 609–631 (cit. on pp. 3, 4, 26)

  34. [34]

    Generalized Stealthy Hyperuniform Processes: Max- imal Rigidity and the Bounded Holes Conjecture

    S. Ghosh and J. L. Lebowitz. “Generalized Stealthy Hyperuniform Processes: Max- imal Rigidity and the Bounded Holes Conjecture”. In:Communications in Math- ematical Physics363.11 (Oct. 2018), pp. 97–110 (cit. on pp. 3, 17, 25, 26)

  35. [35]

    Rigidity and tolerance in point processes: Gaussian ze- ros and Ginibre eigenvalues

    S. Ghosh and Y. Peres. “Rigidity and tolerance in point processes: Gaussian ze- ros and Ginibre eigenvalues”. In:Duke Mathematical Journal166.10 (July 2017), pp. 1789–1858 (cit. on pp. 4, 26)

  36. [36]

    Engineered Hyperuniformity for Directional Light Extraction

    S. Gorsky et al. “Engineered Hyperuniformity for Directional Light Extraction”. In:APL Photonics4 (2019), p. 110801 (cit. on p. 3)

  37. [37]

    Gut.Stopped Random Walks: Limit Theorems and Applications

    A. Gut.Stopped Random Walks: Limit Theorems and Applications. Springer Series in Operations Research and Financial Engineering. New York, NY: Springer New York, 2009 (cit. on p. 100)

  38. [38]

    Transition from Light Diffusion to Localization in Three-Dimensional Amorphous Dielectric Networks near the Band Edge

    J. Haberko, L. S. Froufe-P´ erez, and F. Scheffold. “Transition from Light Diffusion to Localization in Three-Dimensional Amorphous Dielectric Networks near the Band Edge”. In:Nat. Commun.11 (2020), p. 4867 (cit. on p. 3)

  39. [39]

    Central limit theorems for Poisson hyperplane tessellations

    L. Heinrich, H. Schmidt, and V. Schmidt. “Central limit theorems for Poisson hyperplane tessellations”. In:The Annals of Applied Probability16.2 (May 2006), pp. 919–950 (cit. on p. 30)

  40. [40]

    L¨ owner-John ellipsoids

    M. Henk. “L¨ owner-John ellipsoids”. In:Documenta Mathematica(Jan. 2012) (cit. on p. 94)

  41. [41]

    A Stable Marriage of Poisson and Lebesgue

    C. Hoffman, A. E. Holroyd, and Y. Peres. “A Stable Marriage of Poisson and Lebesgue”. In:Annals of Probability34 (2005), pp. 1241–1272 (cit. on p. 53)

  42. [42]

    R. A. Horn and C. R. Johnson.Matrix Analysis. Cambridge University Press, 1985 (cit. on p. 49)

  43. [43]

    Optimal transport between random measures

    M. Huesmann. “Optimal transport between random measures”. In:Annales de l’Institut Henri Poincar´ e, Probabilit´ es et Statistiques52.1 (2016), pp. 196–232 (cit. on pp. 34, 75)

  44. [44]

    The link between hyperuniformity, Coulomb energy and Wasserstein distance to Lebesgue for two-dimensional point processes

    M. Huesmann and T. Lebl´ e. “The link between hyperuniformity, Coulomb energy and Wasserstein distance to Lebesgue for two-dimensional point processes”. In: Probability and Mathematical Physics7 (Jan. 2026), pp. 123–173 (cit. on pp. 3, 7, 73, 74)

  45. [45]

    Optimal transport from Lebesgue to Poisson

    M. Huesmann and K.-T. Sturm. “Optimal transport from Lebesgue to Poisson”. In:The Annals of Probability41.4 (2013), pp. 2426–2478 (cit. on p. 75)

  46. [46]

    Iosevich and E

    A. Iosevich and E. Liflyand.Decay of the Fourier Transform: Analytic and Geo- metric Aspects. Mathematics and Statistics. Springer Basel, 2014 (cit. on p. 84)

  47. [47]

    On a Formula for the Product-Moment Coefficient of any Order of a Normal Frequency Distribution in any Number of Variables

    L. Isserlis. “On a Formula for the Product-Moment Coefficient of any Order of a Normal Frequency Distribution in any Number of Variables”. In:Biometrika 12.1–2 (Nov. 1918), pp. 134–139 (cit. on pp. 66, 68, 69, 71). 109

  48. [48]

    The space D in several variables: random variables and higher mo- ments

    S. Janson. “The space D in several variables: random variables and higher mo- ments”. In:Mathematica Scandinavica127.3 (Nov. 2021) (cit. on p. 14)

  49. [49]

    Kallenberg.Foundations of Modern Probability

    O. Kallenberg.Foundations of Modern Probability. Probability theory and stochas- tic modelling. Springer, 2021 (cit. on pp. 16, 17, 29)

  50. [50]

    Kallenberg.Random Measures, Theory and Applications

    O. Kallenberg.Random Measures, Theory and Applications. Vol. 77. Jan. 2017 (cit. on p. 8)

  51. [51]

    On the Translocation of Masses

    L. Kantorovitch. “On the Translocation of Masses”. In:Management Science5.1 (1958), pp. 1–4 (cit. on p. 13)

  52. [52]

    Khoshnevisan.Multiparameter processes: an introduction to random fields

    D. Khoshnevisan.Multiparameter processes: an introduction to random fields. Sprin- ger monographs in mathematics. New York, Berlin, Heidelberg [u.a.]: Springer, 2002 (cit. on p. 15)

  53. [53]

    New tessellation-based procedure to design perfectly hyperuniform disordered dispersions for materials discovery

    J. Kim and S. Torquato. “New tessellation-based procedure to design perfectly hyperuniform disordered dispersions for materials discovery”. In:Acta Materialia 168 (Apr. 2019), pp. 143–151 (cit. on p. 51)

  54. [54]

    Effect of imperfections on the hyperuniformity of many- body systems

    J. Kim and S. Torquato. “Effect of imperfections on the hyperuniformity of many- body systems”. In:Physical Review B97.55 (Feb. 2018), p. 054105 (cit. on pp. 69, 70)

  55. [55]

    Effect of window shape on the detection of hyperunifor- mity via the local number variance

    J. Kim and S. Torquato. “Effect of window shape on the detection of hyperunifor- mity via the local number variance”. In:Journal of Statistical Mechanics: Theory and Experiment2017.11 (Jan. 2017), p. 013402 (cit. on pp. 17, 21, 84)

  56. [56]

    Invariant transports of sta- tionary random measures: asymptotic variance, hyperuniformity, and examples

    M. A. Klatt, G. Last, L. Lotz, and D. Yogeshwaran. “Invariant transports of sta- tionary random measures: asymptotic variance, hyperuniformity, and examples”. In: arXiv:2506.05907 (June 2025) (cit. on pp. 3, 5, 7–11, 13, 14, 44, 45, 51–53, 56, 65)

  57. [57]

    Wave Propagation and Band Tails of Two-Dimensional Disordered Systems in the Thermodynamic Limit

    M. A. Klatt, P. J. Steinhardt, and S. Torquato. “Wave Propagation and Band Tails of Two-Dimensional Disordered Systems in the Thermodynamic Limit”. In:Proc. Natl. Acad. Sci.119 (2022), e2213633119 (cit. on p. 3)

  58. [58]

    On strongly rigid hyperfluctuating random measures

    M. A. Klatt and G. Last. “On strongly rigid hyperfluctuating random measures”. In:Journal of Applied Probability59.4 (2022), pp. 948–961 (cit. on p. 30)

  59. [59]

    Hyperuniform and rigid stable match- ings

    M. A. Klatt, G. Last, and D. Yogeshwaran. “Hyperuniform and rigid stable match- ings”. In:Random Structures & Algorithms57.22 (Apr. 2020), pp. 439–473 (cit. on p. 3)

  60. [60]

    Stationary random measures: Covariance asymptotics, variance bounds and central limit theorems

    M. Krishnapur and D. Yogeshwaran. “Stationary random measures: Covariance asymptotics, variance bounds and central limit theorems”. In: arXiv:2411.08848 (Nov. 2024) (cit. on pp. 17, 22)

  61. [61]

    Hyperuniform random measures, transport and rigidity

    R. Lachi` eze-Rey. “Hyperuniform random measures, transport and rigidity”. In: arXiv:2510.18392 (Oct. 2025) (cit. on pp. 3, 15, 17, 21, 23, 30, 59)

  62. [62]

    Rigidity of random stationary measures and applications to point processes

    R. Lachi` eze-Rey. “Rigidity of random stationary measures and applications to point processes”. In: arXiv:2409.18519 (Feb. 2025) (cit. on pp. 3, 4, 7, 26, 27, 30, 31, 60). 110

  63. [63]

    Hyperuniformity and optimal transport of point processes

    R. Lachi` eze-Rey and D. Yogeshwaran. “Hyperuniformity and optimal transport of point processes”. In: arXiv:2402.13705 (Mar. 2024) (cit. on pp. 3, 7, 73, 74)

  64. [64]

    Landau and E

    L. Landau and E. Lifshitz.Statistical Physics: Volume 5. Butterworth-Heinemann, 2013 (cit. on p. 70)

  65. [65]

    Last and M

    G. Last and M. Penrose.Lectures on the Poisson Process. Institute of Mathematical Statistics Textbooks. Cambridge University Press, 2018 (cit. on pp. 8, 9)

  66. [66]

    Invariant transports of stationary random measures and mass-stationarity

    G. Last and H. Thorisson. “Invariant transports of stationary random measures and mass-stationarity”. In:The Annals of Probability37.2 (2009), pp. 790–813 (cit. on p. 13)

  67. [67]

    The Two-Dimensional One-Component Plasma Is Hyperuniform

    T. Lebl´ e. “The Two-Dimensional One-Component Plasma Is Hyperuniform”. In: Duke Math. J.175 (2026), pp. 763–901 (cit. on p. 3)

  68. [68]

    Hyperuniform Interfaces in Nonequilibrium Phase Coexistence

    R. Maire, L. Galliano, A. Plati, and L. Berthier. “Hyperuniform Interfaces in Nonequilibrium Phase Coexistence”. In:Phys. Rev. Lett.135 (2025), p. 227102 (cit. on p. 3)

  69. [69]

    Estimating the hyperuniformity exponent of point processes

    G. Mastrilli, B. B laszczyszyn, and F. Lavancier. “Estimating the hyperuniformity exponent of point processes”. In: arXiv:2407.16797 (July 2024) (cit. on pp. 3, 15, 17, 21)

  70. [70]

    Grundlegende Eigenschaften der polynomischen Oper- ationen. Erste Mitteilung

    S. Mazur and W. Orlicz. “Grundlegende Eigenschaften der polynomischen Oper- ationen. Erste Mitteilung”. In:Studia Mathematica5.1 (1934), pp. 50–68 (cit. on p. 57)

  71. [71]

    Newton’s Identities

    D. G. Mead. “Newton’s Identities”. In:The American Mathematical Monthly99.8 (1992), pp. 749–751 (cit. on p. 87)

  72. [72]

    Crack STIT tessellations: characterization of stationary random tessellations stable with respect to iteration

    W. Nagel and V. Weiss. “Crack STIT tessellations: characterization of stationary random tessellations stable with respect to iteration”. In:Advances in Applied Probability37.4 (2005), pp. 859–883 (cit. on pp. 5, 54)

  73. [73]

    Limits of Sequences of Stationary Planar Tessellations

    W. Nagel and V. Weiss. “Limits of Sequences of Stationary Planar Tessellations”. In:Advances in Applied Probability35.1 (2003), pp. 123–138 (cit. on pp. 5, 54)

  74. [74]

    Hyperuniformity of quasicrystals

    E. C. O˘ guz, J. E. S. Socolar, P. J. Steinhardt, and S. Torquato. “Hyperuniformity of quasicrystals”. In:Physical Review B95.55 (Feb. 2017), p. 054119 (cit. on pp. 2, 3, 15)

  75. [75]

    Olevskii and A

    A. Olevskii and A. Ulanovskii. “A Simple Crystalline Measure”. In: arXiv:2006.12037 (June 2020) (cit. on p. 58)

  76. [76]

    Olver, D

    F. Olver, D. Lozier, R. Boisvert, and C. Clark.The NIST Handbook of Mathe- matical Functions. Cambridge University Press, New York, NY, May 2010 (cit. on p. 102)

  77. [77]

    The Pinwheel Tilings of the Plane

    C. Radin. “The Pinwheel Tilings of the Plane”. In:Annals of Mathematics139.3 (1994), pp. 661–702 (cit. on pp. 7, 52)

  78. [78]

    Long-Range Anomalous Decay of the Correlation in Jammed Packings

    P. Rissone, E. I. Corwin, and G. Parisi. “Long-Range Anomalous Decay of the Correlation in Jammed Packings”. In:Phys. Rev. Lett.127 (2021), p. 038001 (cit. on p. 3). 111

  79. [79]

    Hyperuniformity and Number Rigidity of Inflation Tilings

    D. Roca. “Hyperuniformity and Number Rigidity of Inflation Tilings”. In: arXiv: 2310.20517 (Oct. 2023) (cit. on p. 15)

  80. [80]

    Superstable interactions in classical statistical mechanics

    D. Ruelle. “Superstable interactions in classical statistical mechanics”. In:Com- munications in Mathematical Physics18.2 (June 1970), pp. 127–159 (cit. on p. 69)

Showing first 80 references.