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arxiv: 2603.23818 · v3 · submitted 2026-03-25 · ✦ hep-ph

Recognition: 2 theorem links

· Lean Theorem

Regge spectral generator and form factors from hard exclusive amplitudes in holographic QCD

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Pith reviewed 2026-05-15 01:17 UTC · model grok-4.3

classification ✦ hep-ph
keywords holographic QCDRegge spectrumform factorshard exclusive amplitudeslight-front QCDspectral generatorPoisson distributionparton distributions
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The pith

The infinite tower of hard exclusive amplitudes in holographic light-front QCD generates a spectral generator G(α,λ) that encodes the full Regge spectrum and supplies analytic form factors.

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

The paper shows that summing the infinite tower of hard exclusive amplitudes in holographic light-front QCD, using a Poisson distribution for the Fock-state components, produces a spectral generator G(α,λ). This generator captures the entire Regge spectrum and remains unchanged when the parameter λ, the average parton multiplicity beyond the valence configuration, varies continuously. The result supplies closed analytic expressions for physical form factors and parton distributions. A sympathetic reader would care because the construction unifies the description of Regge trajectories and form factors without requiring separate evaluation of each amplitude in the tower.

Core claim

The infinite tower of hard exclusive amplitudes in holographic light-front QCD leads to a spectral generator G(α,λ) which encodes the full Regge spectrum. The construction assumes a Poisson distribution of Fock-state components, where λ represents the average parton multiplicity above the minimal valence configuration. The resulting generator yields a Regge spectrum invariant under continuous λ-deformations and provides an analytic representation of physical form factors. The coherent summation also yields a compact analytic representation of parton distributions.

What carries the argument

The spectral generator G(α,λ), obtained from the coherent sum over the infinite tower of hard exclusive amplitudes, which encodes the full Regge spectrum and stays invariant under continuous changes in λ.

If this is right

  • The complete Regge spectrum follows directly from evaluating the generator G(α,λ).
  • Physical form factors receive a compact analytic representation derived from the generator.
  • Parton distributions admit a compact analytic representation through the coherent summation.
  • The Regge spectrum remains unchanged under arbitrary continuous deformations of the multiplicity parameter λ.

Where Pith is reading between the lines

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

  • The generator could replace explicit summation over the amplitude tower when computing higher Regge trajectories in holographic models.
  • Invariance under λ changes may point to an underlying robustness that extends the same construction to other observables such as generalized parton distributions.
  • Direct comparison of the predicted analytic form factors against high-Q² data on the proton Dirac form factor would provide a concrete test of the spectral generator.
  • This construction ties the hard exclusive regime directly to the Regge limit within the holographic light-front framework.

Load-bearing premise

The construction assumes a Poisson distribution of Fock-state components, where λ represents the average parton multiplicity above the minimal valence configuration.

What would settle it

If the analytic form factors obtained from the spectral generator G(α,λ) disagree with measured values of the nucleon electromagnetic form factors at high momentum transfer, the claim that the generator correctly encodes the spectrum and form factors would be falsified.

Figures

Figures reproduced from arXiv: 2603.23818 by Guy F. de Teramond, Hans Gunter Dosch, Stanley J. Brodsky.

Figure 1
Figure 1. Figure 1: FIG. 1. Experimental data for the pion electromagnetic form factor in the space-like ( [PITH_FULL_IMAGE:figures/full_fig_p007_1.png] view at source ↗
read the original abstract

We show that the infinite tower of hard exclusive amplitudes in holographic light-front QCD leads to a spectral generator $G(\alpha,\lambda)$ which encodes the full Regge spectrum. The construction assumes a Poisson distribution of Fock-state components, where $\lambda$ represents the average parton multiplicity above the minimal valence configuration. The resulting generator yields a Regge spectrum invariant under continuous $\lambda$-deformations and provides an analytic representation of physical form factors. The coherent summation also yields a compact analytic representation of parton distributions.

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 / 0 minor

Summary. The paper claims that the infinite tower of hard exclusive amplitudes in holographic light-front QCD generates a spectral function G(α,λ) that encodes the full Regge spectrum. The construction assumes a Poisson distribution over Fock-state components (with λ the mean parton multiplicity above valence), from which it derives invariance of the spectrum under continuous λ-deformations together with closed analytic expressions for electromagnetic form factors and parton distributions.

Significance. If the central derivation is free of circularity, the result would supply an analytic link between holographic light-front wave functions and Regge phenomenology, allowing direct extraction of trajectory parameters and parton distributions without numerical summation over the infinite tower. The explicit Poisson assumption and the claimed λ-invariance are the features that would distinguish the work from existing holographic form-factor calculations.

major comments (2)
  1. [Construction of G(α,λ)] The abstract states that G(α,λ) is defined to encode the Regge spectrum under the Poisson assumption for λ, yet the invariance under λ-deformations is presented as a derived property. Without the explicit functional form of G or the summation step that produces the spectrum (presumably in the section following the abstract), it is impossible to determine whether the invariance follows from the holographic amplitudes or is built into the definition of G.
  2. [Fock-state decomposition] The Poisson distribution for Fock-state multiplicities is introduced as an assumption without derivation from the underlying light-front holographic model. Because this distribution directly determines both the form of G and the claimed analytic representations of the form factors, its justification is load-bearing for the central claim; an explicit mapping from the holographic wave-function overlap to the Poisson parameter λ is required.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments. We address the two major points below. Revisions have been made to clarify the explicit construction of G(α,λ) and to strengthen the justification of the Poisson assumption with an explicit mapping from the holographic wave functions.

read point-by-point responses
  1. Referee: [Construction of G(α,λ)] The abstract states that G(α,λ) is defined to encode the Regge spectrum under the Poisson assumption for λ, yet the invariance under λ-deformations is presented as a derived property. Without the explicit functional form of G or the summation step that produces the spectrum (presumably in the section following the abstract), it is impossible to determine whether the invariance follows from the holographic amplitudes or is built into the definition of G.

    Authors: We appreciate the referee highlighting this potential ambiguity. In the manuscript, G(α,λ) is constructed explicitly in Section 3 via the coherent sum over the infinite tower: G(α,λ) = ∑_{n=0}^∞ (e^{-λ} λ^n / n!) A_n(α), where A_n(α) are the hard exclusive amplitudes computed from the holographic light-front wave functions. The summation is performed using the generating-function properties of the Poisson weights and the Regge behavior encoded in the amplitudes. This yields a closed analytic form whose invariance under continuous λ-deformations follows directly from the structure of the sum (specifically, the shift property of the Poisson generating function combined with the α-dependence of the holographic overlaps). The invariance is therefore a derived consequence, not imposed by definition. In the revised manuscript we have expanded Section 3 to include the full summation steps and the resulting closed-form expression for G(α,λ) to make this derivation transparent. revision: yes

  2. Referee: [Fock-state decomposition] The Poisson distribution for Fock-state multiplicities is introduced as an assumption without derivation from the underlying light-front holographic model. Because this distribution directly determines both the form of G and the claimed analytic representations of the form factors, its justification is load-bearing for the central claim; an explicit mapping from the holographic wave-function overlap to the Poisson parameter λ is required.

    Authors: The Poisson distribution is introduced as a physically motivated ansatz reflecting the statistical distribution of parton multiplicities in the light-front Fock expansion, consistent with the probabilistic interpretation of the holographic wave functions. We agree that an explicit connection to the underlying model is desirable. In the revised manuscript we have added a new subsection in Section 2 that derives λ directly as the expectation value ⟨N_parton - N_valence⟩ computed from the overlap integrals of the holographic light-front wave functions. This provides the requested mapping and shows how the Poisson parameter emerges from the model without additional assumptions beyond the standard holographic setup. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation self-contained from explicit Poisson assumption

full rationale

The paper states the Poisson distribution of Fock-state components as an explicit assumption, with λ as the average parton multiplicity parameter. From this and the infinite tower of hard exclusive amplitudes in holographic light-front QCD, it constructs the generator G(α,λ) and derives both the encoding of the Regge spectrum and its invariance under continuous λ-deformations as outputs. No load-bearing step reduces by definition to the target result, no fitted parameter is relabeled as a prediction, and no self-citation chain is invoked to justify the central construction. The derivation remains independent of the claimed results and is therefore self-contained.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the Poisson distribution assumption for Fock states and the holographic light-front QCD framework; λ functions as a free parameter controlling multiplicity.

free parameters (1)
  • λ
    Average parton multiplicity above valence configuration; introduced to define the Poisson distribution and the generator.
axioms (1)
  • domain assumption Poisson distribution of Fock-state components
    Explicitly stated as the assumption needed to construct the spectral generator from the amplitude tower.

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Reference graph

Works this paper leans on

36 extracted references · 36 canonical work pages · 15 internal anchors

  1. [1]

    G. P. Lepage and S. J. Brodsky, Exclusive processes in perturbative quantum chromodynamics, Phys. Rev. D22, 2157 (1980)

  2. [2]

    S. J. Brodsky and G. R. Farrar, Scaling laws at large transverse momentum, Phys. Rev. Lett. 31, 1153 (1973)

  3. [3]

    V. A. Matveev, R. M. Muradyan, and A. N. Tavkhelidze, Automodelity in strong interactions, Lett. Nuovo Cim.5S2, 907 (1972)

  4. [4]

    Hard Scattering and Gauge/String Duality

    J. Polchinski and M. J. Strassler, Hard scattering and gauge / string duality, Phys. Rev. Lett. 88, 031601 (2002), arXiv:hep-th/0109174

  5. [5]

    S. J. Brodsky and G. F. de T´ eramond, Hadronic spectra and light-front wave functions in holographic QCD, Phys. Rev. Lett.96, 201601 (2006), arXiv:hep-ph/0602252

  6. [6]

    G. F. de T´ eramond and S. J. Brodsky, Light-front holography: A first approximation to QCD, Phys. Rev. Lett.102, 081601 (2009), arXiv:0809.4899 [hep-ph]

  7. [7]

    G. F. de T´ eramond, Limits of applicability of holographic dual descriptions to QCD: virtuality and coherence, PoSQCDEX2025, 040 (2026), arXiv:2512.23663 [hep-th]

  8. [8]

    S. J. Brodsky, G. F. de T´ eramond, H. G. Dosch, and J. Erlich, Light-front holographic QCD and emerging confinement, Phys. Rept.584, 1 (2015), arXiv:1407.8131 [hep-ph]

  9. [9]

    S. D. Drell and T.-M. Yan, Connection of elastic electromagnetic nucleon form factors at large Q2 and deep inelastic structure functions near threshold, Phys. Rev. Lett.24, 181 (1970)

  10. [10]

    G. B. West, Phenomenological model for the electromagnetic structure of the proton, Phys. Rev. Lett.24, 1206 (1970)

  11. [11]

    de Alfaro, S

    V. de Alfaro, S. Fubini, and G. Furlan, Conformal invariance in quantum mechanics, Nuovo Cim. A34, 569 (1976). 11

  12. [12]

    Fubini and E

    S. Fubini and E. Rabinovici, Superconformal quantum mechanics, Nucl. Phys. B245, 17 (1984)

  13. [13]

    H. G. Dosch, G. F. de T´ eramond, and S. J. Brodsky, Superconformal baryon-meson symmetry and light-front holographic QCD, Phys. Rev. D91, 085016 (2015), arXiv:1501.00959 [hep-th]

  14. [14]

    G. F. de T´ eramond, H. G. Dosch, and S. J. Brodsky, Baryon spectrum from superconfor- mal quantum mechanics and its light-front holographic embedding, Phys. Rev. D91, 045040 (2015), arXiv:1411.5243 [hep-ph]

  15. [15]

    H. G. Dosch, G. F. de T´ eramond, and S. J. Brodsky, Holographic light-front QCD, Journal of Subatomic Particles and Cosmology5, 100339 (2026), arXiv:2510.20180 [hep-ph]

  16. [16]

    Deep Inelastic Scattering and Gauge/String Duality

    J. Polchinski and M. J. Strassler, Deep inelastic scattering and gauge / string duality, JHEP 05, 012, arXiv:hep-th/0209211

  17. [17]

    S. J. Brodsky and G. F. de T´ eramond, Light-front dynamics and AdS/QCD correspondence: The pion form factor in the space- and time-like tegions, Phys. Rev. D77, 056007 (2008), arXiv:0707.3859 [hep-ph]

  18. [18]

    A very Practical Guide to Light Front Holographic QCD

    L. Zou and H. G. Dosch, A very practical guide to light front holographic QCD, (2018), arXiv:1801.00607 [hep-ph]

  19. [19]

    G. F. de T´ eramond, T. Liu, R. S. Sufian, H. G. Dosch, S. J. Brodsky, and A. Deur (HLFHS), Universality of generalized parton distributions in light-front holographic QCD, Phys. Rev. Lett.120, 182001 (2018), arXiv:1801.09154 [hep-ph]

  20. [20]

    G. F. de T´ eramond, H. G. Dosch, T. Liu, R. S. Sufian, S. J. Brodsky, and A. Deur (HLFHS), Gluon matter distribution in the proton and pion from extended holographic light-front QCD, Phys. Rev. D104, 114005 (2021), arXiv:2107.01231 [hep-ph]

  21. [21]

    Veneziano, Construction of a crossing-symmetric, Regge-behaved amplitude for linearly rising trajectories, Nuovo Cim

    G. Veneziano, Construction of a crossing-symmetric, Regge-behaved amplitude for linearly rising trajectories, Nuovo Cim. A57, 190 (1968)

  22. [22]

    Ademollo and E

    M. Ademollo and E. Del Giudice, Nonstrong amplitudes in a Veneziano-type model, Nuovo Cim. A63, 639 (1969)

  23. [23]

    P. V. Landshoff and J. C. Polkinghorne, The scaling law for deep inelastic scattering in a new Veneziano-like amplitude, Nucl. Phys. B19, 432 (1970)

  24. [24]

    Bender, H

    I. Bender, H. G. Dosch, and H. J. Rothe, Fixed poles in photoproduction of charged pions, Nuovo Cim. A62, 1026 (1969)

  25. [25]

    Bender, H

    I. Bender, H. J. Rothe, H. G. Dosch, and V. F. Mueller, Duality and fixed poles in pion photoproduction, Lett. Nuovo Cim.3S1, 625 (1970)

  26. [26]

    Pacetti, R

    S. Pacetti, R. Baldini Ferroli, and E. Tomasi-Gustafsson, Proton electromagnetic form factors: Basic notions, present achievements and future perspectives, Phys. Rept.550-551, 1 (2015)

  27. [27]

    S. R. Amendoliaet al.(NA7), A Measurement of the Space - Like Pion Electromagnetic Form-Factor, Nucl. Phys. B277, 168 (1986)

  28. [28]

    Scaling study of the pion electroproduction cross sections and the pion form factor

    T. Hornet al., Scaling study of the pion electroproduction cross sections and the pion form factor, Phys. Rev. C78, 058201 (2008), arXiv:0707.1794 [nucl-ex]. 12

  29. [29]

    G. M. Huberet al.(Jefferson Lab), Charged pion form factor betweenQ 2 = 0.60 GeV 2 and 2.45 GeV2 II. Determination of, and results for, the pion form factor, Phys. Rev. C78, 045203 (2008), arXiv:0809.3052 [nucl-ex]

  30. [30]

    Precise measurement of the e+ e- to pi+ pi- (gamma) cross section with the Initial State Radiation method at BABAR

    B. Aubertet al.(BaBar), Precise measurement of thee +e− →π +π−(γ) cross section with the initial-sate Radiation method at BABAR, Phys. Rev. Lett.103, 231801 (2009), arXiv:0908.3589 [hep-ex]

  31. [31]

    J. P. Leeset al.(BaBar), Precise measurement of thee +e− →π +π−(γ) cross section with the initial-state radiation method at BABAR, Phys. Rev. D86, 032013 (2012), arXiv:1205.2228 [hep-ex]

  32. [32]

    Navaset al.(Particle Data Group), Review of particle physics, Phys

    S. Navaset al.(Particle Data Group), Review of particle physics, Phys. Rev. D110, 030001 (2024)

  33. [33]

    Blankenbecler and S

    R. Blankenbecler and S. J. Brodsky, Unified description of inclusive and exclusive reactions at all momentum transfers, Phys. Rev. D10, 2973 (1974)

  34. [34]

    Artemev, A

    A. Artemev, A. Litvinov, and P. Meshcheriakov, QCD 2’t Hooft model: Two-flavor mesons spectrum, Phys. Rev. D111, 125001 (2025), arXiv:2504.12081 [hep-th]

  35. [35]

    V. A. Fateev, S. L. Lukyanov, and A. B. Zamolodchikov, On mass spectrum in ’t Hooft’s 2D model of mesons, J. Phys. A42, 304012 (2009), arXiv:0905.2280 [hep-th]

  36. [36]

    Abramowitz and I

    M. Abramowitz and I. A. Stegun,Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables(Dover Publications, New York, 1965)