On the amplitude expansion of gluon correlators in textrm{AdS}₄
Pith reviewed 2026-06-26 07:07 UTC · model grok-4.3
The pith
Tree-level gluon correlators in AdS4 decompose into sums over energy poles whose residues are flat-space amplitudes at all multiplicities.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Tree-level gluon correlators in AdS4 admit a natural expansion in terms of flat-space scattering amplitudes at all multiplicities. In particular, every n-point correlator can be decomposed into a sum over energy poles whose residues are flat-space amplitudes. The n-point amplitude encodes the flat-space limit while curvature corrections are captured by lower-point amplitudes with merged external data. The merging of external polarizations is recursively defined via an AdS analogue of the Berends-Giele currents, giving rise to all-multiplicity formulae which we verify against Feynman diagram computations up to five points. Crucially, the approach works at the level of full correlators rather
What carries the argument
The AdS analogue of the Berends-Giele currents, which recursively merge external polarizations to produce the curvature corrections at each multiplicity.
If this is right
- The leading term in each energy-pole residue is precisely the flat-space n-point amplitude.
- All curvature corrections at n points are expressed using amplitudes with fewer external legs whose data have been merged.
- Repeated application of the recursion produces explicit closed-form expressions for correlators of any multiplicity.
- The decomposition applies directly to the complete correlator, bypassing the need to sum individual diagrams.
Where Pith is reading between the lines
- The same pole structure may apply to other fields or to higher-dimensional AdS spaces once an appropriate recursive current is identified.
- Holographic computations could become simpler by importing known flat-space amplitudes and only evaluating the merged lower-point corrections.
- A mismatch at six or higher points would indicate that additional non-recursive curvature terms are required.
Load-bearing premise
The recursive AdS analogue of the Berends-Giele currents correctly captures every curvature correction and reproduces the full correlator for arbitrary n.
What would settle it
An explicit six-point gluon correlator computed both by direct Feynman diagrams and by the recursive pole expansion, if the two results disagree, would falsify the claim.
read the original abstract
We show that tree-level gluon correlators in $\textrm{AdS}_4$ admit a natural expansion in terms of flat-space scattering amplitudes at all multiplicities. In particular, every $n$-point correlator can be decomposed into a sum over energy poles whose residues are flat-space amplitudes. The $n$-point amplitude encodes the flat-space limit while curvature corrections are captured by lower-point amplitudes with merged external data. The merging of external polarizations is recursively defined via an AdS analogue of the Berends-Giele currents, giving rise to all-multiplicity formulae which we verify against Feynman diagram computations up to five points. Crucially, our approach works at the level of full correlators rather than individual diagrams, providing an elegant and transparent alternative to conventional approaches for computing correlators in anti-de Sitter space.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that tree-level gluon correlators in AdS₄ admit a natural expansion in flat-space scattering amplitudes at all multiplicities. Every n-point correlator decomposes into a sum over energy poles whose residues are flat-space amplitudes; the n-point term encodes the flat-space limit while curvature corrections arise from lower-point amplitudes with merged external data. The merging is defined recursively via an AdS analogue of the Berends-Giele currents, yielding explicit all-multiplicity formulae that are verified against Feynman diagrams up to five points. The method is presented as operating at the level of full correlators rather than individual diagrams.
Significance. If the recursive construction is shown to hold generally, the result would be significant as it supplies an elegant recursive construction that reduces AdS correlator computation to known flat-space amplitudes plus a merging procedure, providing a transparent alternative to direct diagrammatic calculations in curved space. Credit is due for the full-correlator perspective and the explicit all-multiplicity formulae, even though their generality is currently supported only by limited verification.
major comments (2)
- [Abstract] Abstract: the central all-multiplicity claim rests on the assertion that the AdS Berends-Giele recursion captures every curvature correction for arbitrary n, yet the manuscript states that the resulting formulae are verified against Feynman diagrams only up to five points, with no inductive argument, structural proof, or statement of the precise matching criterion provided to establish that the recursion exhausts all AdS corrections beyond n=5.
- [Abstract] Abstract: the verification is described only as 'against Feynman diagram computations up to five points' without error bars, a precise matching criterion, or confirmation that the check covers the full correlator (rather than selected components), which is load-bearing for assessing whether the recursion reproduces the complete AdS result.
Simulated Author's Rebuttal
We thank the referee for the detailed report and constructive feedback on our manuscript. We address the two major comments point by point below, agreeing where the presentation requires clarification and outlining the revisions we will make.
read point-by-point responses
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Referee: [Abstract] Abstract: the central all-multiplicity claim rests on the assertion that the AdS Berends-Giele recursion captures every curvature correction for arbitrary n, yet the manuscript states that the resulting formulae are verified against Feynman diagrams only up to five points, with no inductive argument, structural proof, or statement of the precise matching criterion provided to establish that the recursion exhausts all AdS corrections beyond n=5.
Authors: The AdS Berends-Giele recursion is constructed precisely so that each step merges lower-point data to account for all curvature corrections at the given multiplicity; the all-multiplicity formulae follow directly from iterating this procedure. The recursive definition itself supplies the structural argument that every correction is captured, without requiring an additional inductive step. We acknowledge, however, that the manuscript does not spell out this reasoning explicitly or provide a formal statement of the matching criterion. We will revise the abstract and the relevant sections to clarify that the formulae are obtained by recursive application of the AdS currents, which by construction exhausts the curvature corrections at every n, and to state the precise sense in which the five-point checks validate the implementation. revision: partial
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Referee: [Abstract] Abstract: the verification is described only as 'against Feynman diagram computations up to five points' without error bars, a precise matching criterion, or confirmation that the check covers the full correlator (rather than selected components), which is load-bearing for assessing whether the recursion reproduces the complete AdS result.
Authors: We agree that the current description of the verification is insufficiently detailed. The checks were performed on the full correlators by comparing the complete set of energy-pole residues and the curvature corrections obtained from the recursion against independent Feynman-diagram results, with exact symbolic agreement required. In the revised manuscript we will expand this description, specify the matching criterion (coefficient-by-coefficient equality in the energy-pole expansion), confirm that the entire correlator was compared at each multiplicity, and note that the computations are exact (hence no error bars). revision: yes
Circularity Check
No circularity: recursion and flat-space inputs are independent; verification is explicit up to n=5
full rationale
The derivation defines an AdS analogue of Berends-Giele currents as a new recursive merging rule for external data, takes known flat-space amplitudes as external inputs, and checks the resulting pole-residue formulae against Feynman diagrams only up to five points. No equation reduces a claimed prediction to a fitted parameter or to a self-referential definition; no load-bearing step rests on a self-citation chain. The all-multiplicity statement is an unproven extrapolation rather than a circular reduction, so the construction remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
invented entities (1)
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AdS analogue of Berends-Giele currents
no independent evidence
Forward citations
Cited by 1 Pith paper
-
Dirichlet, Neumann, Mixed and self-dual holography: (self-dual) Yang--Mills theory II
Derives bulk and boundary propagators and computes 3- and 4-point correlators for YM, CS and SDYM in AdS/CFT with multiple boundary conditions to relate their observables.
Reference graph
Works this paper leans on
-
[1]
in terms of merged external data. Together, these two observations allow us to establish all-multiplicity formulae for gluon correlators in AdS4 in terms of flat- space amplitude data alone. An important feature of our approach is that it operates at the level of full correlators, rather than individual Feynman diagrams. The amplitude expansion structure ...
Pith/arXiv arXiv 2026
-
[2]
J. M. Maldacena, Non-Gaussian features of primordial fluctuations in single field inflationary models, JHEP05, 013, arXiv:astro-ph/0210603
-
[3]
A. Bzowski, P. McFadden, and K. Skenderis, Implications 7 of conformal invariance in momentum space, JHEP03, 111, arXiv:1304.7760 [hep-th]
-
[4]
Raju, New Recursion Relations and a Flat Space Limit for AdS/CFT Correlators, Phys
S. Raju, New Recursion Relations and a Flat Space Limit for AdS/CFT Correlators, Phys. Rev. D85, 126009 (2012), arXiv:1201.6449 [hep-th]
Pith/arXiv arXiv 2012
-
[5]
F.A.BerendsandW.T.Giele,RecursiveCalculationsfor Processes with n Gluons, Nucl. Phys. B306, 759 (1988)
1988
-
[6]
D. Baumann, D. Green, A. Joyce, E. Pajer, G. L. Pimentel, C. Sleight, and M. Taronna, Snowmass White Paper: The Cosmological Bootstrap, SciPost Phys. Comm. Rep.2024, 1 (2024), arXiv:2203.08121 [hep-th]
arXiv 2024
-
[7]
The interpretation in terms of energy is more transparent in de Sitter space, where the bulk direction is timelike and the boundary is Euclidean
-
[8]
L. J. Dixon, Calculating scattering amplitudes efficiently, inTheoretical Advanced Study Institute in Elementary Particle Physics (TASI 95): QCD and Beyond(1996) pp. 539–584, arXiv:hep-ph/9601359
Pith/arXiv arXiv 1996
-
[9]
N. Arkani-Hamed, P. Benincasa, and A. Postnikov, Cosmological Polytopes and the Wavefunction of the Universe, arXiv preprint (2017), arXiv:1709.02813 [hep- th]
Pith/arXiv arXiv 2017
-
[10]
S. Albayrak, C. Chowdhury, and S. Kharel, Study of momentum space scalar amplitudes in AdS spacetime, Phys. Rev. D101, 124043 (2020), arXiv:2001.06777 [hep- th]
arXiv 2020
-
[11]
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, 071 (2021), arXiv:2005.04234 [hep-th]
arXiv 2021
-
[12]
N. Arkani-Hamed, D. Baumann, H. Lee, and G. L. Pimentel, The Cosmological Bootstrap: Inflationary CorrelatorsfromSymmetriesandSingularities,JHEP04, 105, arXiv:1811.00024 [hep-th]
-
[13]
H. Goodhew, S. Jazayeri, and E. Pajer, The Cosmological Optical Theorem, JCAP04, 021, arXiv:2009.02898 [hep- th]
arXiv 2009
-
[14]
S. Jazayeri, E. Pajer, and D. Stefanyszyn, From locality and unitarity to cosmological correlators, JHEP10, 065, arXiv:2103.08649 [hep-th]
-
[15]
S. Melville and E. Pajer, Cosmological Cutting Rules, JHEP05, 249, arXiv:2103.09832 [hep-th]
-
[16]
A Mathematica notebook with these comparisons is attached to the arXiv submission
-
[17]
H. Liu and A. A. Tseytlin, On four point functions in the CFT / AdS correspondence, Phys. Rev. D59, 086002 (1999), arXiv:hep-th/9807097
Pith/arXiv arXiv 1999
-
[18]
Raju, Recursion Relations for AdS/CFT Correlators, Phys
S. Raju, Recursion Relations for AdS/CFT Correlators, Phys. Rev. D83, 126002 (2011), arXiv:1102.4724 [hep- th]
Pith/arXiv arXiv 2011
-
[19]
J. M. Maldacena and G. L. Pimentel, On graviton non-Gaussianities during inflation, JHEP09, 045, arXiv:1104.2846 [hep-th]
-
[20]
S. Albayrak and S. Kharel, Towards the higher point holographic momentum space amplitudes, JHEP02, 040, arXiv:1810.12459 [hep-th]
-
[21]
In AdS this corresponds to a non-covariant gauge- choice
Note that we are referring to Lorenz gauge in half of flat space. In AdS this corresponds to a non-covariant gauge- choice
-
[22]
C. Armstrong, A. E. Lipstein, and J. Mei, Color/kinematics duality in AdS 4, JHEP02, 194, arXiv:2012.02059 [hep-th]
arXiv 2012
-
[23]
S. Albayrak, C. Chowdhury, and S. Kharel, New relation for Witten diagrams, JHEP10, 274, arXiv:1904.10043 [hep-th]
arXiv 1904
-
[24]
S. J. Parke and T. R. Taylor, An Amplitude fornGluon Scattering, Phys. Rev. Lett.56, 2459 (1986)
1986
-
[25]
A. Hodges, Eliminating spurious poles from gauge- theoretic amplitudes, JHEP05, 135, arXiv:0905.1473 [hep-th]
-
[26]
T. Adamo, M. Bullimore, L. Mason, and D. Skinner, Scattering Amplitudes and Wilson Loops in Twistor Space, J. Phys. A44, 454008 (2011), arXiv:1104.2890 [hep-th]
Pith/arXiv arXiv 2011
-
[27]
R. Bittleston, G. Bogna, S. Heuveline, A. Kmec, L. Mason, and D. Skinner, On AdS 4 deformations of celestial symmetries, JHEP07, 010, arXiv:2403.18011 [hep-th]
-
[28]
D. Baumann, G. Mathys, G. L. Pimentel, and F. Rost, A new twist on spinning (A)dS correlators, JHEP01, 202, arXiv:2408.02727 [hep-th]
-
[29]
M. Arundine, D. Baumann, M. H. G. Lee, G. L. Pimentel, and F. Rost, The Cosmological Grassmannian, arXiv (2026), arXiv:2602.07117 [hep-th]
Pith/arXiv arXiv 2026
-
[30]
S. Albayrak, S. Kharel, and D. Meltzer, On duality of color and kinematics in (A)dS momentum space, JHEP 03, 249, arXiv:2012.10460 [hep-th]
arXiv 2012
-
[31]
C. Armstrong, H. Goodhew, A. Lipstein, and J. Mei, Graviton trispectrum from gluons, JHEP08, 206, arXiv:2304.07206 [hep-th]
-
[32]
A. Lipstein and S. Nagy, Self-Dual Gravity and Color- Kinematics Duality in AdS4, Phys. Rev. Lett.131, 081501 (2023), arXiv:2304.07141 [hep-th]
arXiv 2023
-
[33]
C. Chowdhury, G. Doran, A. Lipstein, R. Monteiro, S. Nagy, and K. Singh, Light-cone actions and correlators of self-dual theories in AdS4, JHEP01, 172, arXiv:2411.04172 [hep-th]
-
[34]
Gomez, R
H. Gomez, R. Lipinski Jusinskas, A. Lipstein, and C. Lopez-Arcos, to appear, arXiv (2026)
2026
-
[35]
N. Arkani-Hamed, Y. Bai, S. He, and G. Yan, Scattering Forms and the Positive Geometry of Kinematics, Color and the Worldsheet, JHEP05, 096, arXiv:1711.09102 [hep-th]
- [36]
-
[37]
N. Arkani-Hamed, C. Figueiredo, and F. Vazão, Cosmohedra, JHEP11, 029, arXiv:2412.19881 [hep-th]
-
[38]
A. A. Rosly and K. G. Selivanov, On amplitudes in selfdual sector of Yang-Mills theory, Phys. Lett.B399, 135 (1997), arXiv:hep-th/9611101 [hep-th]
Pith/arXiv arXiv 1997
-
[39]
A. A. Rosly and K. G. Selivanov, Gravitational SD perturbiner, arXiv (1997), arXiv:hep-th/9710196 [hep- th]
Pith/arXiv arXiv 1997
-
[40]
C. R. Mafra and O. Schlotterer, Solution to the nonlinear field equations of ten dimensional supersymmetric Yang-Mills theory, Phys. Rev.D92, 066001 (2015), arXiv:1501.05562 [hep-th]
Pith/arXiv arXiv 2015
-
[41]
C. Armstrong, H. Gomez, R. Lipinski Jusinskas, A. Lipstein, and J. Mei, New recursion relations for tree- level correlators in anti–de Sitter spacetime, Phys. Rev. D106, L121701 (2022), arXiv:2209.02709 [hep-th]
arXiv 2022
-
[42]
E. Skvortsov and R. Van Dongen, Dirichlet, Neumann, Mixed and self-dual holography: (self-dual) Yang-Mills theory, arXiv (2026), arXiv:2602.21658 [hep-th]
arXiv 2026
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