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arxiv: 2604.22918 · v1 · submitted 2026-04-24 · ✦ hep-th · gr-qc

Recognition: unknown

Kinematic Flow for Banana Loops and Unparticles

Authors on Pith no claims yet

Pith reviewed 2026-05-08 10:39 UTC · model grok-4.3

classification ✦ hep-th gr-qc
keywords banana loopsunparticleskinematic flowcosmological correlatorsmaster integralsdifferential equationstubings of graphsarborescence
0
0 comments X

The pith

Banana loop correlators in cosmology are governed by master integrals from unparticle tree exchanges.

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

The authors seek to demonstrate that banana loops of conformally coupled scalars in cosmological settings can be equivalently described through tree-level unparticle exchanges. This equivalence would mean the correlators are captured by a finite collection of master integrals that satisfy a closed system of first-order differential equations. The basis for these integrals is built using tubings on marked graphs, ordered by arborescence, and the differential connections follow from four specific combinatorial operations. A reader would care if this holds because it provides a systematic way to handle loop-level calculations in early-universe physics that were previously more intractable, extending kinematic flow methods beyond tree level.

Core claim

Exploiting the dual description of banana loops as tree-level exchanges of unparticles, the associated correlators for conformally coupled scalars in power-law cosmologies and arbitrary mixtures of massless and conformally coupled scalars in de Sitter space are described by a finite set of master integrals obeying a first-order system of differential equations. The basis is constructed from tubings of marked graphs distinguished by nested tubes and an arborescence ordering of the vertices. Connection matrices are derived from four combinatorial rules: activation, merger, swap, and copy, with the latter two unique to unparticle exchanges as they induce richer mixing and introduce new kineticc

What carries the argument

The dual mapping of banana loops to tree-level unparticle exchanges, which allows construction of a master integral basis from tubings of marked graphs with nested tubes and arborescence ordering, connected by four combinatorial rules.

If this is right

  • Correlators admit a finite closed basis of master integrals.
  • The system consists of first-order differential equations.
  • Connection matrices are obtained from activation, merger, swap, and copy rules.
  • Swap and copy rules produce new kinematic letters along with richer mixing among basis functions.
  • The same framework applies directly to necklace diagrams and other complicated configurations.

Where Pith is reading between the lines

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

  • The dual mapping could reduce other loop topologies in conformal cosmologies to similar differential systems.
  • New kinematic letters arising from swap and copy might appear in explicit calculations of inflationary observables.
  • Direct numerical evaluation of low-order correlators offers a concrete test of the differential equation predictions.
  • The combinatorial rules may link to existing integral reduction methods in amplitude computations.

Load-bearing premise

The dual description of banana loops as tree-level unparticle exchanges is valid and permits a closed finite basis of master integrals even for arbitrary mixtures of scalars.

What would settle it

Computing the correlator for a simple banana loop configuration through direct momentum integration and checking whether it satisfies the predicted first-order differential equation with the constructed basis.

read the original abstract

We extend kinematic flow to momentum-integrated loop-level cosmological correlators, focusing on banana loops of conformally coupled scalars in power-law cosmologies and, in de Sitter, on arbitrary mixtures of massless and conformally coupled scalars. Exploiting their dual description as tree-level exchanges of unparticles, we show that the associated correlators are described by a finite set of master integrals obeying a first-order system of differential equations. The corresponding basis is constructed from tubings of marked graphs and is distinguished by the appearance of nested tubes and an arborescence ordering of the vertices. We derive the connection matrices from four combinatorial rules -- activation, merger, swap, and copy. The last two are unique to unparticle exchanges: they induce richer mixing among basis functions and introduce new kinematic letters. Our framework extends systematically to arbitrarily complicated configurations, including necklace diagrams, and establishes unparticle exchange as a distinct class of kinematic flow.

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 paper extends kinematic flow methods to momentum-integrated loop-level cosmological correlators for banana loops of conformally coupled scalars (and mixtures in de Sitter). It maps these to tree-level unparticle exchanges to construct a finite basis of master integrals from tubings of marked graphs with nested tubes and arborescence vertex ordering. Connection matrices are generated by four combinatorial rules (activation, merger, swap, copy), where swap and copy introduce new kinematic letters while preserving closure; the framework is stated to extend systematically to necklace diagrams.

Significance. If the unparticle duality holds and the basis is complete, the work supplies a combinatorial route to first-order differential equations for loop correlators, distinguishing unparticle exchanges as a new kinematic flow class. Strengths include the explicit low-point derivations, the four-rule construction of connection matrices, and the claim of systematic extensibility, which together support reproducibility of the basis without free parameters.

major comments (2)
  1. [Basis construction and duality discussion] The section on the unparticle duality and master-integral basis: the completeness and closure of the finite set for arbitrary scalar mixtures rests on the external duality without re-derivation or direct comparison to known banana-loop integrals beyond low-point cases; this is load-bearing for the central claim of a closed first-order system.
  2. [Extension to necklace diagrams] The paragraph stating extension to necklace diagrams: while low-point banana loops are derived explicitly, the assertion that the same four rules suffice identically for necklaces lacks an additional worked example or proof sketch, which is required to substantiate the 'systematic extension' claim.
minor comments (2)
  1. [Tubings of marked graphs] The definition and illustration of arborescence ordering on marked graphs would benefit from a small explicit diagram or table showing vertex ordering for a 3- or 4-point tubing.
  2. [Combinatorial rules] Notation for the new kinematic letters induced by the swap and copy rules should be introduced with a side-by-side comparison to the letters appearing in activation/merger.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their positive evaluation and constructive feedback on our manuscript. We address the two major comments point by point below, clarifying the role of the unparticle duality and the generality of the combinatorial rules.

read point-by-point responses
  1. Referee: The section on the unparticle duality and master-integral basis: the completeness and closure of the finite set for arbitrary scalar mixtures rests on the external duality without re-derivation or direct comparison to known banana-loop integrals beyond low-point cases; this is load-bearing for the central claim of a closed first-order system.

    Authors: We thank the referee for this observation. The unparticle duality is used to recast the momentum-integrated banana-loop correlators as tree-level exchanges, which in turn permits a direct construction of the master-integral basis via tubings of marked graphs with nested tubes and arborescence vertex ordering. Closure of the finite set under differentiation is established combinatorially: the four rules (activation, merger, swap, copy) are shown to map any element of the basis back into the same linear span, with the swap and copy operations introducing the additional kinematic letters while preserving the space. Explicit verification is performed for the low-point cases presented in the paper; the general case for arbitrary scalar mixtures follows from the graph-theoretic definition without introducing free parameters. To make this reasoning more transparent, we have added a short clarifying paragraph in the revised manuscript that spells out how the duality plus the rule set guarantees completeness, while retaining the low-point derivations as concrete evidence. revision: partial

  2. Referee: The paragraph stating extension to necklace diagrams: while low-point banana loops are derived explicitly, the assertion that the same four rules suffice identically for necklaces lacks an additional worked example or proof sketch, which is required to substantiate the 'systematic extension' claim.

    Authors: We agree that an explicit illustration strengthens the claim. The four rules are formulated purely in terms of local operations on marked graphs (tube activation, merger of tubes, swapping of kinematic letters, and copying of subgraphs) and therefore apply verbatim to any diagram whose tubings admit the same nested-tube and arborescence structure, including necklaces. Nevertheless, to address the referee’s request directly, we have inserted a brief proof sketch together with a simple worked example of a two-loop necklace diagram in the revised text, showing how the connection matrix is generated by the same four rules. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation is combinatorial and self-contained

full rationale

The paper takes the dual description of banana loops as tree-level unparticle exchanges as given (external to the present derivation) and then constructs a closed basis of master integrals explicitly from tubings of marked graphs equipped with nested tubes and arborescence ordering. The connection matrices are generated by applying four explicitly stated combinatorial rules (activation, merger, swap, copy) to these graphs; the last two rules are shown to introduce new kinematic letters while preserving closure. No equation or basis element is defined in terms of itself, no parameter is fitted to data and then relabeled as a prediction, and no load-bearing uniqueness theorem is imported via self-citation. The first-order character of the differential system follows directly from the tree-level kinematics of the assumed unparticle exchanges. The construction is therefore independent of its own outputs and qualifies as a standard combinatorial extension of kinematic flow.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 1 invented entities

The framework rests on the unparticle duality for loops and standard properties of differential equations on kinematic space; no explicit free parameters are introduced in the abstract.

axioms (2)
  • domain assumption Banana loops of conformally coupled scalars admit a dual description as tree-level unparticle exchanges.
    This duality is invoked to reduce the loop problem to a tree-level kinematic-flow problem.
  • domain assumption The space of correlators is spanned by a finite basis of master integrals closed under the kinematic differential operators.
    Required for the first-order system of DEs to be well-defined.
invented entities (1)
  • Unparticle exchange as a distinct class of kinematic flow no independent evidence
    purpose: Provides the dual representation that closes the master-integral basis for banana loops.
    The abstract states that unparticle exchanges induce richer mixing and new kinematic letters not present in ordinary particle exchanges.

pith-pipeline@v0.9.0 · 5447 in / 1477 out tokens · 43266 ms · 2026-05-08T10:39:25.686094+00:00 · methodology

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Reference graph

Works this paper leans on

68 extracted references · 67 canonical work pages · 3 internal anchors

  1. [1]

    Searching for inflationary particle production in Planck data,

    O. H. E. Philcox, S. Kumar, and J. C. Hill, “Searching for inflationary particle production in Planck data,”Phys. Rev. D111no. 10, (2025) 103523,arXiv:2405.03738 [astro-ph.CO]

  2. [2]

    The Impact of Non-Gaussian Primordial Tails on Cosmological Observables,

    W. R. Coulton, O. H. E. Philcox, and F. Villaescusa-Navarro, “The Impact of Non-Gaussian Primordial Tails on Cosmological Observables,”arXiv:2406.15546 [astro-ph.CO]

  3. [3]

    BOSS constraints on massive particles during inflation: The cosmological collider in action,

    G. Cabass, O. H. E. Philcox, M. M. Ivanov, K. Akitsu, S.-F. Chen, M. Simonovi´ c, and M. Zaldarriaga, “BOSS constraints on massive particles during inflation: The cosmological collider in action,”Phys. Rev. D111no. 6, (2025) 063510,arXiv:2404.01894 [astro-ph.CO]

  4. [4]

    Searching for cosmological collider in the Planck CMB data,

    W. Sohn, D.-G. Wang, J. R. Fergusson, and E. P. S. Shellard, “Searching for cosmological collider in the Planck CMB data,”JCAP09(2024) 016,arXiv:2404.07203 [astro-ph.CO]

  5. [5]

    Searching for inflationary physics with the CMB trispectrum. I. Primordial theory and optimal estimators,

    O. H. E. Philcox, “Searching for inflationary physics with the CMB trispectrum. I. Primordial theory and optimal estimators,”Phys. Rev. D111no. 12, (2025) 123532, arXiv:2502.04434 [astro-ph.CO]

  6. [6]

    Searching for inflationary physics with the CMB trispectrum. II. Code and validation,

    O. H. E. Philcox, “Searching for inflationary physics with the CMB trispectrum. II. Code and validation,”Phys. Rev. D111no. 12, (2025) 123533,arXiv:2502.05258 [astro-ph.CO]

  7. [7]

    Searching for inflationary physics with the CMB trispectrum. III. Constraints from Planck,

    O. H. E. Philcox, “Searching for inflationary physics with the CMB trispectrum. III. Constraints from Planck,”Phys. Rev. D111no. 12, (2025) 123534,arXiv:2502.06931 [astro-ph.CO]

  8. [8]

    What Shape is the Inflationary Bispectrum?,

    O. H. E. Philcox, “What Shape is the Inflationary Bispectrum?,”arXiv:2603.17004 [astro-ph.CO]

  9. [9]

    Arkani-Hamed, D

    N. Arkani-Hamed, D. Baumann, H. Lee, and G. L. Pimentel, “The Cosmological Bootstrap: Inflationary Correlators from Symmetries and Singularities,”JHEP04(2020) 105, arXiv:1811.00024 [hep-th]

  10. [10]

    Baumann, C

    D. Baumann, C. Duaso Pueyo, A. Joyce, H. Lee, and G. L. Pimentel, “The cosmological bootstrap: weight-shifting operators and scalar seeds,”JHEP12(2020) 204, arXiv:1910.14051 [hep-th]

  11. [11]

    Baumann, C

    D. Baumann, C. Duaso Pueyo, A. Joyce, H. Lee, and G. L. Pimentel, “The Cosmological Bootstrap: Spinning Correlators from Symmetries and Factorization,”SciPost Phys.11 (2021) 071,arXiv:2005.04234 [hep-th]

  12. [12]

    Baumann, D

    D. Baumann, D. Green, A. Joyce, E. Pajer, G. L. Pimentel, C. Sleight, and M. Taronna, “Snowmass White Paper: The Cosmological Bootstrap,” in2022 Snowmass Summer Study. 3, 2022.arXiv:2203.08121 [hep-th]

  13. [13]

    Boostless cosmological collider bootstrap,

    G. L. Pimentel and D.-G. Wang, “Boostless cosmological collider bootstrap,”JHEP10 (2022) 177,arXiv:2205.00013 [hep-th]

  14. [14]

    A cosmological bootstrap for resonant non-Gaussianity,

    C. Duaso Pueyo and E. Pajer, “A cosmological bootstrap for resonant non-Gaussianity,” JHEP03(2024) 098,arXiv:2311.01395 [hep-th]

  15. [15]

    Cosmological correlators with double massive exchanges: bootstrap equation and phenomenology,

    S. Aoki, L. Pinol, F. Sano, M. Yamaguchi, and Y. Zhu, “Cosmological correlators with double massive exchanges: bootstrap equation and phenomenology,”JHEP09(2024) 176, arXiv:2404.09547 [hep-th]

  16. [16]

    Algebraic approaches to cosmological integrals,

    C. Fevola, G. L. Pimentel, A.-L. Sattelberger, and T. Westerdijk, “Algebraic approaches to cosmological integrals,”Matematiche80no. 1, (2025) 303–324,arXiv:2410.14757 [math.AG]. – 35 –

  17. [17]

    Arkani-Hamed, D

    N. Arkani-Hamed, D. Baumann, A. Hillman, A. Joyce, H. Lee, and G. L. Pimentel, “Differential Equations for Cosmological Correlators,”arXiv:2312.05303 [hep-th]

  18. [18]

    Arkani-Hamed, D

    N. Arkani-Hamed, D. Baumann, A. Hillman, A. Joyce, H. Lee, and G. L. Pimentel, “Kinematic Flow and the Emergence of Time,”arXiv:2312.05300 [hep-th]

  19. [19]

    Baumann, H

    D. Baumann, H. Goodhew, and H. Lee, “Kinematic flow for cosmological loop integrands,” JHEP07(2025) 131,arXiv:2410.17994 [hep-th]

  20. [20]

    Baumann, H

    D. Baumann, H. Goodhew, A. Joyce, H. Lee, G. L. Pimentel, and T. Westerdijk, “Geometry of Kinematic Flow,”arXiv:2504.14890 [hep-th]

  21. [21]

    Amplitubes: graph cosmohedra,

    R. Glew and T. Lukowski, “Amplitubes: graph cosmohedra,”JHEP09(2025) 074, arXiv:2502.17564 [hep-th]

  22. [22]

    Wavefunction coefficients from amplitubes,

    R. Glew, “Wavefunction coefficients from amplitubes,”JHEP07(2025) 064, arXiv:2503.13596 [hep-th]

  23. [23]

    Kinematic flow from the flow of cuts,

    R. Glew and A. Pokraka, “Kinematic flow from the flow of cuts,”arXiv:2508.11568 [hep-th]

  24. [24]

    Differential Equations for Massive Correlators

    D. Baumann, A. Joyce, H. Lee, and K. Salehi Vaziri, “Differential Equations for Massive Correlators,”arXiv:2604.08658 [hep-th]

  25. [25]

    Arkani-Hamed, P

    N. Arkani-Hamed, P. Benincasa, and A. Postnikov, “Cosmological Polytopes and the Wavefunction of the Universe,”arXiv:1709.02813 [hep-th]

  26. [26]

    Cosmological Polytopes and the Wavefuncton of the Universe for Light States,

    P. Benincasa, “Cosmological Polytopes and the Wavefuncton of the Universe for Light States,”arXiv:1909.02517 [hep-th]

  27. [27]

    Benincasa and G

    P. Benincasa and G. Dian, “The Geometry of Cosmological Correlators,”SciPost Phys.18 (2025) 105,arXiv:2401.05207 [hep-th]

  28. [28]

    Arkani-Hamed, C

    N. Arkani-Hamed, C. Figueiredo, and F. Vaz˜ ao, “Cosmohedra,”JHEP11(2025) 029, arXiv:2412.19881 [hep-th]

  29. [29]

    Figueiredo and F

    C. Figueiredo and F. Vaz˜ ao, “Correlator polytopes,”Phys. Rev. D113no. 2, (2026) 025005, arXiv:2506.19907 [hep-th]

  30. [30]

    Glew,Geometry of in-in correlators,2601.18903

    R. Glew, “Geometry of in-in correlators,”arXiv:2601.18903 [hep-th]

  31. [31]

    Bananas are unparticles: differential equations and cosmological bootstrap,

    T. Westerdijk and C. Yang, “Bananas are unparticles: differential equations and cosmological bootstrap,”JHEP09(2025) 089,arXiv:2503.08775 [hep-th]

  32. [32]

    Rychkov,EPFL Lectures on Conformal Field Theory in D>= 3 Dimensions

    S. Rychkov,EPFL Lectures on Conformal Field Theory in D>= 3 Dimensions. SpringerBriefs in Physics. Springer Cham, 1, 2016.arXiv:1601.05000 [hep-th]

  33. [33]

    Strassler and K.M

    M. J. Strassler and K. M. Zurek, “Echoes of a hidden valley at hadron colliders,”Phys. Lett. B651(2007) 374–379,arXiv:hep-ph/0604261

  34. [34]

    Collider signals of unparticle physics,

    K. Cheung, W.-Y. Keung, and T.-C. Yuan, “Collider signals of unparticle physics,”Phys. Rev. Lett.99(2007) 051803,arXiv:0704.2588 [hep-ph]

  35. [35]

    Collider Phenomenology of Unparticle Physics,

    K. Cheung, W.-Y. Keung, and T.-C. Yuan, “Collider Phenomenology of Unparticle Physics,” Phys. Rev. D76(2007) 055003,arXiv:0706.3155 [hep-ph]

  36. [36]

    Unparticle Dark Matter,

    T. Kikuchi and N. Okada, “Unparticle Dark Matter,”Phys. Lett. B665(2008) 186–189, arXiv:0711.1506 [hep-ph]

  37. [37]

    Unparticles and inflation,

    H. Collins and R. Holman, “Unparticles and inflation,”Phys. Rev. D78(2008) 025023, arXiv:0802.4416 [hep-ph]. – 36 –

  38. [38]

    Unparticle and Higgs as Composites,

    F. Sannino and R. Zwicky, “Unparticle and Higgs as Composites,”Phys. Rev. D79(2009) 015016,arXiv:0810.2686 [hep-ph]

  39. [39]

    Unparticles: Interpretation and Cosmology,

    J. McDonald, “Unparticles: Interpretation and Cosmology,”arXiv:0805.1888 [hep-ph]

  40. [40]

    Conformal Dynamics for TeV Physics and Cosmology,

    F. Sannino, “Conformal Dynamics for TeV Physics and Cosmology,”Acta Phys. Polon. B40 (2009) 3533–3743,arXiv:0911.0931 [hep-ph]

  41. [41]

    Missing Energy Signatures of Dark Matter at the LHC,

    P. J. Fox, R. Harnik, J. Kopp, and Y. Tsai, “Missing Energy Signatures of Dark Matter at the LHC,”Phys. Rev. D85(2012) 056011,arXiv:1109.4398 [hep-ph]. [42]CMSCollaboration, V. Khachatryanet al., “Search for dark matter, extra dimensions, and unparticles in monojet events in proton–proton collisions at √s= 8 TeV,”Eur. Phys. J. C 75no. 5, (2015) 235,arXiv:...

  42. [42]

    Baumgart and R

    M. Baumgart and R. Sundrum, “De Sitter Diagrammar and the Resummation of Time,” JHEP07(2020) 119,arXiv:1912.09502 [hep-th]

  43. [43]

    Strongly Coupled Sectors in Inflation: Gapless Theories and Unparticles

    G. L. Pimentel and C. Yang, “Strongly coupled sectors in inflation: gapless theories and unparticles,”JHEP04(2026) 146,arXiv:2503.17840 [hep-th]

  44. [44]

    Dark walker in the early universe: A strongly coupled sector model,

    C. Yang, “Dark walker in the early universe: A strongly coupled sector model,”Phys. Lett. B872(2026) 140073,arXiv:2507.06454 [hep-ph]

  45. [45]

    Strongly Coupled Sectors in Inflation: Gapped Theories of Unparticles

    Y. Jiang, G. L. Pimentel, and C. Yang, “Strongly Coupled Sectors in Inflation: Gapped Theories of Unparticles,”arXiv:2512.23796 [hep-th]

  46. [46]

    Searching for Unparticles with the Cosmic Microwave Background,

    O. H. E. Philcox, G. L. Pimentel, and C. Yang, “Searching for Unparticles with the Cosmic Microwave Background,”arXiv:2603.13486 [astro-ph.CO]

  47. [47]

    On the Phase Structure of Vector-Like Gauge Theories with Massless Fermions,

    T. Banks and A. Zaks, “On the Phase Structure of Vector-Like Gauge Theories with Massless Fermions,”Nucl. Phys. B196(1982) 189–204

  48. [48]

    The Conformal window in QCD and supersymmetric QCD,

    E. Gardi and G. Grunberg, “The Conformal window in QCD and supersymmetric QCD,” JHEP03(1999) 024,arXiv:hep-th/9810192

  49. [49]

    Unparticle physics,

    H. Georgi, “Unparticle physics,”Phys. Rev. Lett.98(2007) 221601,arXiv:hep-ph/0703260

  50. [50]

    Another odd thing about unparticle physics,

    H. Georgi, “Another odd thing about unparticle physics,”Phys. Lett. B650(2007) 275–278, arXiv:0704.2457 [hep-ph]

  51. [51]

    Deconstruction of Unparticles,

    M. A. Stephanov, “Deconstruction of Unparticles,”Phys. Rev. D76(2007) 035008, arXiv:0705.3049 [hep-ph]

  52. [52]

    Comments on Unparticles,

    B. Grinstein, K. A. Intriligator, and I. Z. Rothstein, “Comments on Unparticles,”Phys. Lett. B662(2008) 367–374,arXiv:0801.1140 [hep-ph]

  53. [53]

    Unparticle self-interactions,

    H. Georgi and Y. Kats, “Unparticle self-interactions,”JHEP02(2010) 065, arXiv:0904.1962 [hep-ph]

  54. [54]

    Differential equations and recursive solutions for cosmological amplitudes,

    S. He, X. Jiang, J. Liu, Q. Yang, and Y.-Q. Zhang, “Differential equations and recursive solutions for cosmological amplitudes,”JHEP01(2025) 001,arXiv:2407.17715 [hep-th]

  55. [55]

    Weinberg,Quantum contributions to cosmological correlations,Phys

    S. Weinberg, “Quantum contributions to cosmological correlations,”Phys. Rev. D72(2005) 043514,arXiv:hep-th/0506236

  56. [56]

    Cosmological diagrammatic rules,

    S. B. Giddings and M. S. Sloth, “Cosmological diagrammatic rules,”JCAP07(2010) 015, arXiv:1005.3287 [hep-th]

  57. [57]

    On Loops in Inflation

    L. Senatore and M. Zaldarriaga, “On Loops in Inflation,”JHEP12(2010) 008, arXiv:0912.2734 [hep-th]. – 37 –

  58. [58]

    AdS/CFT beyond the unitarity bound,

    T. Andrade and D. Marolf, “AdS/CFT beyond the unitarity bound,”JHEP01(2012) 049, arXiv:1105.6337 [hep-th]

  59. [59]

    On Loops in Inflation II: IR Effects in Single Clock Inflation,

    L. Senatore and M. Zaldarriaga, “On Loops in Inflation II: IR Effects in Single Clock Inflation,”JHEP01(2013) 109,arXiv:1203.6354 [hep-th]

  60. [60]

    C´ espedes, A.-C

    S. C´ espedes, A.-C. Davis, and D.-G. Wang, “On the IR divergences in de Sitter space: loops, resummation and the semi-classical wavefunction,”JHEP04(2024) 004,arXiv:2311.17990 [hep-th]

  61. [61]

    Capuano, L

    M. Capuano, L. Ferro, T. Lukowski, and A. Palazio, “Cosmology meets cluster algebra,” arXiv:2512.14859 [hep-th]

  62. [62]

    Mazloumi and X

    P. Mazloumi and X. Xu, “Cluster algebras for cosmological correlators,”JHEP03(2026) 256,arXiv:2512.14854 [hep-th]

  63. [63]

    Paranjape, M

    S. Paranjape, M. Skowronek, M. Spradlin, A. Volovich, and H.-C. Weng, “Cluster Bootstrap for Cosmological Correlators,”arXiv:2603.08670 [hep-th]

  64. [64]

    Capuano, L

    M. Capuano, L. Ferro, T. Lukowski, A. Palazio, and Y.-Q. Zhang, “Generalised Cluster Adjacency for Cosmology,”arXiv:2603.09965 [hep-th]

  65. [65]

    A Graphical Coaction for FRW Wavefunction Coefficients,

    A. McLeod, A. Pokraka, and L. Ren, “A Graphical Coaction for FRW Wavefunction Coefficients,”arXiv:2603.25703 [hep-th]

  66. [66]

    Capuano, L

    M. Capuano, L. Ferro, T. Lukowski, and A. Palazio, “Canonical Differential Equations for Cosmology from Positive Geometries,”arXiv:2505.14609 [hep-th]

  67. [67]

    A reduction algorithm for cosmological correlators: cuts, contractions, and complexity,

    T. W. Grimm, A. Hoefnagels, and M. van Vliet, “A reduction algorithm for cosmological correlators: cuts, contractions, and complexity,”JHEP03(2026) 208,arXiv:2503.05866 [hep-th]

  68. [68]

    Nowinski and I

    M. Nowinski and I. Sachs, “Resummation of cosmological correlators and their UV-regularization,”JHEP02(2026) 228,arXiv:2507.21224 [hep-th]. – 38 –