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arxiv: 2605.26024 · v1 · pith:PNYNATQNnew · submitted 2026-05-25 · 🧮 math-ph · hep-th· math.KT· math.MP

Field theory of mathfrak{su}(n): the absence of non-zero scatterings

Pith reviewed 2026-06-29 19:09 UTC · model grok-4.3

classification 🧮 math-ph hep-thmath.KTmath.MP
keywords su(n) formshomological perturbation theoryscattering amplitudestree-level diagramsgauge symmetriesfield theoryhigher productsinteraction vertex
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The pith

Homological perturbation theory applied to su(n) forms shows no scattering amplitudes from trivalent tree-level diagrams except the interaction vertex.

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

The paper treats su(n) forms as a finite-dimensional toy model for field theories that include gauge symmetries. It uses homological perturbation theory to prove that all trivalent tree diagrams beyond the basic vertex give zero scattering amplitudes, and this holds for every n. A reader would care because the result limits what perturbative interactions can occur in the model and shows how the same underlying algebra behaves differently when the field space is enlarged. The contrast with the non-vanishing higher products obtained after transfer to a larger space highlights that the choice of field space controls which interactions survive.

Core claim

Relying on homological perturbation theory, we show that there are no scattering amplitudes with trivalent tree-level diagrams, except for the interaction vertex, thus extending a known argument to arbitrary n. In contrast to this, we show how to obtain non-trivial higher products when transferring to a larger space of fields.

What carries the argument

Homological perturbation theory applied directly to the finite-dimensional su(n) forms, which isolates the vanishing of all but the three-point vertex in tree-level diagrams.

If this is right

  • Only the three-point interaction vertex contributes to tree-level scattering; all other trivalent diagrams cancel.
  • The perturbative expansion of the theory remains minimal at tree level for every value of n.
  • Transferring the algebraic structure to an enlarged field space produces non-trivial higher-order operations that were absent in the original space.
  • The same su(n) algebra yields different interaction content depending on the dimension of the field space chosen.

Where Pith is reading between the lines

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

  • The vanishing result could be checked by direct low-order calculations for small n to confirm consistency with the general argument.
  • Similar transfer techniques might be applied to other finite-dimensional Lie algebra models to generate controlled higher interactions.
  • If the pattern holds, it suggests that enlarging the field space is a systematic way to introduce complexity without changing the underlying algebra.
  • The absence of extra tree diagrams may simplify numerical or symbolic checks of the model for arbitrary n.

Load-bearing premise

Homological perturbation theory applies directly to the finite-dimensional su(n) forms without additional hidden assumptions that would alter the vanishing result for tree-level diagrams.

What would settle it

An explicit computation of any trivalent tree-level scattering amplitude for a chosen n greater than 3 that yields a non-zero value would falsify the vanishing claim.

read the original abstract

We inspect $\mathfrak{su}(n)$ forms, providing greater detail for $n=2,3$, as a toy model for a field theory in finite dimensions and with gauge symmetries. Relying on homological perturbation theory, we show that there are no scattering amplitudes with trivalent tree-level diagrams, except for the interaction vertex, thus extending a known argument of Cattaneo--Mn\"{e}v to arbitrary $n$. In contrast to this, we show how to obtain non-trivial higher products when transferring to a larger space of fields.

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

0 major / 1 minor

Summary. The manuscript claims that homological perturbation theory applied to finite-dimensional su(n) forms yields vanishing of all non-trivial trivalent tree-level scattering amplitudes except the basic interaction vertex itself. This extends the Cattaneo-Mněv argument to arbitrary n, with explicit algebraic checks provided for n=2 and n=3; the authors further contrast the vanishing result with the appearance of non-trivial higher products after transfer to an enlarged field space.

Significance. If the central derivation holds, the work supplies a clean algebraic demonstration that tree-level scattering vanishes in this finite-dimensional gauge-theoretic toy model, crediting the direct application of the homological perturbation lemma for a parameter-free result that generalizes prior work. The explicit low-n verifications and the controlled contrast with the enlarged space strengthen the claim by showing how the vanishing depends on the choice of field space.

minor comments (1)
  1. [Sections detailing n=2,3 checks] The explicit computations for n=2 and n=3 would benefit from a short table listing the chosen basis elements for the su(n) forms and the resulting differential and product maps, to make the verification steps fully reproducible from the text alone.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their accurate summary of our manuscript and for the positive assessment leading to a recommendation of minor revision. No specific major comments or requests for changes were provided in the report.

Circularity Check

0 steps flagged

No significant circularity; extends external prior argument

full rationale

The manuscript applies homological perturbation theory directly to finite-dimensional su(n) forms, deriving the vanishing of non-trivial trivalent tree-level scattering amplitudes (except the basic vertex) for general n via algebraic computation, with explicit verification for n=2,3 and contrast to the non-vanishing case after field-space transfer. The central claim is framed as an explicit extension of the external Cattaneo-Mněv argument rather than a self-referential fit, renormalization, or self-citation chain. No step reduces by construction to its own inputs, and the derivation remains self-contained against the stated external benchmark.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the applicability of homological perturbation theory to the su(n) model and on the validity of the finite-dimensional toy model as a proxy for gauge symmetries.

axioms (1)
  • domain assumption Homological perturbation theory can be applied to su(n) forms to compute scattering amplitudes.
    The proof method stated in the abstract relies on this technique.

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discussion (0)

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Reference graph

Works this paper leans on

35 extracted references · 29 canonical work pages · 12 internal anchors

  1. [1]

    Factorization Algebras in Quantum Field The- ory,

    K. Costello and O. Gwilliam, “Factorization Algebras in Quantum Field The- ory,” Cambridge University Press, 2021, ISBN 978-1-316-67866-4, 978-1-107-16315-7 doi:10.1017/9781316678664

  2. [2]

    Lectures on Batalin-Vilkovisky formalism and its applications in topological quantum field theory

    P. Mnëv, “Lectures on Batalin-Vilkovisky formalism and its applications in topological quan- tum field theory,” [arXiv:1707.08096 [math-ph]]

  3. [3]

    Batalin–Vilkovisky quantization of fuzzy field theories,

    H. Nguyen, A. Schenkel and R. J. Szabo, “Batalin–Vilkovisky quantization of fuzzy field theories,” Lett. Math. Phys.111(2021) no.6, 149 doi:10.1007/s11005-021-01490-2 [arXiv:2107.02532 [hep-th]]

  4. [4]

    Cohomology theory of Lie groups and Lie algebras

    C. Chevalley and S. Eilenberg “Cohomology theory of Lie groups and Lie algebras”, Trans. Am. Math. Soc, 63(1), (1948) pp. 85–124. doi:10.1090/s0002-9947-1948-0024908-8

  5. [5]

    Symmetry Factors of Feynman Diagrams and the Ho- mological Perturbation Lemma,

    C. Sämann and E. Sfinarolakis, “Symmetry Factors of Feynman Diagrams and the Ho- mological Perturbation Lemma,” JHEP12(2020), 088 doi:10.1007/JHEP12(2020)088 [arXiv:2009.12616 [hep-th]]

  6. [6]

    𝐿∞-Algebras of Classical Field The- ories and the Batalin-Vilkovisky Formalism,

    B. Jurčo, L. Raspollini, C. Sämann and M. Wolf, “𝐿∞-Algebras of Classical Field The- ories and the Batalin-Vilkovisky Formalism,” Fortsch. Phys.67(2019) no.7, 1900025 doi:10.1002/prop.201900025 [arXiv:1809.09899 [hep-th]]

  7. [7]

    Fieldtheoryandmechanicsfromhomologyandhomotopy,

    L’.Ravas,“Fieldtheoryandmechanicsfromhomologyandhomotopy,”MasterThesis(2025), Comenius university Bratislava

  8. [8]

    Notes from the winter school Geometry and Physics

    C. Sämann, “Notes from the winter school Geometry and Physics”, Srní (2020), at this url

  9. [9]

    Quantum Field Theory and the Jones Polynomial,

    E. Witten, “Quantum Field Theory and the Jones Polynomial,” Commun. Math. Phys.121 (1989), 351-399 doi:10.1007/BF01217730

  10. [10]

    On the perturbation lemma, and deformations

    M. Crainic, “On the perturbation lemma, and deformations,” [arXiv:math/0403266 [math.AT]]

  11. [11]

    Real homotopy theory of Kähler manifolds,

    P. Deligne, P. Griffiths, J. Morgan, D. Sullivan, “Real homotopy theory of Kähler manifolds,” Inventiones mathematicae,29(1975), 245-274 doi:10.1007/BF01389853 . 23 Field theory ofsu(𝑛): the absence of non-zero scatteringsEugenia Boffo

  12. [12]

    New N=2 Superconformal Field Theories in Four Dimensions

    P.C.Argyres,M.R.Plesser,N.SeibergandE.Witten,“NewN=2superconformalfieldtheories in four-dimensions,” Nucl. Phys. B461(1996), 71-84 doi:10.1016/0550-3213(95)00671-0 [arXiv:hep-th/9511154 [hep-th]]

  13. [13]

    RelativisticSMatrixofDynamicalSystemswithBosonand FermionConstraints,

    I.A.BatalinandG.A.Vilkovisky,“RelativisticSMatrixofDynamicalSystemswithBosonand FermionConstraints,”Phys.Lett.B69(1977),309-312doi:10.1016/0370-2693(77)90553-6

  14. [14]

    LagrangianRelationsandQuantum𝐿 ∞ Algebras,

    B.Jurčo,J.PulmannandM.Zika,“LagrangianRelationsandQuantum𝐿 ∞ Algebras,”Com- mun.Math.Phys.406(2025)no.6,143doi:10.1007/s00220-025-05290-w[arXiv:2401.06110 [math-ph]]

  15. [15]

    Loop Amplitudes and Quantum Homotopy Algebras,

    B. Jurčo, T. Macrelli, C. Sämann and M. Wolf, “Loop Amplitudes and Quantum Homotopy Algebras,”JHEP07(2020),003doi:10.1007/JHEP07(2020)003[arXiv:1912.06695[hep-th]]

  16. [16]

    Algebraic operads,

    J.-L. Loday, and B. Vallette, “Algebraic operads," Berlin, (2012) Springer

  17. [17]

    Ein Satz über die Wirkungsräume geschlossener Liescher Grup- pen,

    H. Hopf and H. Samelson, “Ein Satz über die Wirkungsräume geschlossener Liescher Grup- pen,”CommentariimathematiciHelvetici,13(1940/41)240-251http://eudml.org/doc/ 138771

  18. [18]

    How to derive Feynman diagrams for finite-dimensional integrals directly from the BV formalism,

    O. Gwilliam and T. Johnson-Freyd, “How to derive Feynman diagrams for finite-dimensional integrals directly from the BV formalism,” [arXiv:1202.1554 [math-ph]]

  19. [19]

    Remarks on Chern-Simons invariants

    A. S. Cattaneo and P. Mnëv, “Remarks on Chern-Simons invariants,” Commun. Math. Phys. 293(2010), 803-836 doi:10.1007/s00220-009-0959-1 [arXiv:0811.2045 [math.QA]]

  20. [20]

    Renormalization and Effective Field Theory,

    K. Costello, “Renormalization and Effective Field Theory,” (2011), doi:10.1090/surv/170

  21. [21]

    Transferring A∞ (strongly homotopy associative) structures,

    M. Markl “Transferring A∞ (strongly homotopy associative) structures,” Proceedings of the 25th Winter School ”Geometry and Physics”. (2006),http://dml.cz/dmlcz/701773

  22. [22]

    Which homotopy algebras come from transfer?,

    M. Markl and C. L. Rogers, “Which homotopy algebras come from transfer?,” Proc. Amer. Math. Soc. 150 (2022), 975-990 doi:10.1090/proc/15710 [arxiv:2006.00072]

  23. [23]

    Clifford Algebras and Lie Theory,

    E. Meinrenken, “Clifford Algebras and Lie Theory,” Springer Berlin, Heidelberg (2013), doi:10.1007/978-3-642-36216-3

  24. [24]

    The Partition Function of Degenerate Quadratic Functional and Ray-Singer Invariants,

    A. S. Schwarz, “The Partition Function of Degenerate Quadratic Functional and Ray-Singer Invariants,” Lett. Math. Phys.2(1978), 247-252 doi:10.1007/BF00406412

  25. [25]

    Young tableaux and homotopy commutative algebras

    M.Dubois-VioletteandT.Popov,“YoungTableauxandHomotopyCommutativeAlgebras,”Lie Theory and Its Applications in Physics. Springer Proceedings in Mathematics and Statistics, vol 36. Springer [arxiv:1202.2230 [math.QA]]

  26. [26]

    Transferring homotopy commutative algebraic structures

    X. Z. Cheng and E. Getzler, “Transferring homotopy commutative algebraic structures”, Journal of Pure and Applied Algebra 212, 2535 (2008) [arXiv:math/0610912 [math.AT]]

  27. [27]

    Hochschild-Pirashvili homology on suspensions and representations of $Out(F_n)$

    V. Turchin and T. Willwacher, “Hochschild-Pirashvili homology on suspensions and repre- sentationsof𝑂𝑢𝑡(𝐹 𝑛),”Ann.Sci.ÉcoleNorm.Sup.52,761(2019)doi:10.24033/asens.2396 [arXiv:1507.08483 [math.AT]] 24 Field theory ofsu(𝑛): the absence of non-zero scatteringsEugenia Boffo

  28. [28]

    Deformation theory with homotopy algebra structures on tensor products

    D. Robert-Nicoud, “Deformation Theory with Homotopy Algebra Structures on Tensor Prod- ucts,”, Doc. Math. 23, 189 (2018) doi:10.4171/DM/617 [arXiv:1702.02194 [math.QA]]

  29. [29]

    Perturbative aspects of the Chern-Simons topological quantum field theory,

    D. Bar-Natan, “Perturbative aspects of the Chern-Simons topological quantum field theory,” Ph.D. thesis Princeton U. (1991) UMI-91-35830

  30. [30]

    Notes on simplicial BF theory

    P. Mnëv, “Notes on simplicial BF theory,” Mosc. Math. J.9(2009), 371–410 doi:10.17323/1609-4514-2009-9-2-371-410 [arXiv:hep-th/0610326 [hep-th]]

  31. [31]

    Odd Chern-Simons Theory, Lie Algebra Cohomology and Characteristic Classes

    J.QiuandM.Zabzine,“OddChern-SimonsTheory,LieAlgebraCohomologyandCharacter- istic Classes,” Commun. Math. Phys.300(2010), 789-833 doi:10.1007/s00220-010-1102-z [arXiv:0912.1243 [hep-th]]

  32. [32]

    The (secret?) homological algebra of the Batalin-Vilkovisky approach

    J.Stasheff,“The(Secret?) homologicalalgebraoftheBatalin-Vilkoviskyapproach,”Contemp. Math.219(1998), 195-210 doi:10.1090/conm/219/03076 [arXiv:hep-th/9712157 [hep-th]]

  33. [33]

    Homotopy Algebras in String Field Theory,

    I. Sachs, “Homotopy Algebras in String Field Theory,” Fortsch. Phys.67(2019) no.8-9, 1910013 doi:10.1002/prop.201910013 [arXiv:1903.02870 [hep-th]]

  34. [34]

    Closed String Field Theory: Quantum Action and the BV Master Equation

    B.Zwiebach,“Closedstringfieldtheory: QuantumactionandtheB-Vmasterequation,”Nucl. Phys.B390(1993),33-152doi:10.1016/0550-3213(93)90388-6[arXiv:hep-th/9206084[hep- th]]

  35. [35]

    Perspectives on the pure spinor super- field formalism,

    R. Eager, F. Hahner, I. Saberi and B. R. Williams, “Perspectives on the pure spinor super- field formalism,” J. Geom. Phys.180(2022), 104626 doi:10.1016/j.geomphys.2022.104626 [arXiv:2111.01162 [hep-th]]. 25