Note on hidden zeros and expansions of tree-level amplitudes
Pith reviewed 2026-05-23 04:22 UTC · model grok-4.3
The pith
Hidden zeros in tree-level amplitudes of Yang-Mills, gravity and related theories arise from zeros of bi-adjoint scalar amplitudes via universal expansions.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Universal expansions that map amplitudes of Yang-Mills, NLSM, sGal, DBI and gravity onto bi-adjoint scalar amplitudes show that the hidden zeros of the former are inherited from zeros of the latter. The scalar zeros are established by direct inspection of the amplitude expressions. For unordered amplitudes such as those of gravity, the kinematic conditions inducing zeros introduce potential divergences in propagators; the expansions make the cancellation of these divergences manifest through the structure of the summed terms.
What carries the argument
Universal expansions of tree-level amplitudes that expand amplitudes of different theories to those of bi-adjoint scalar theory.
If this is right
- Zeros of all listed amplitudes are proved once the bi-adjoint scalar zeros are known.
- Any kinematic configuration satisfying the zero condition forces the expanded amplitudes to vanish.
- For gravity the expansions guarantee that apparent propagator divergences cancel exactly at the zero loci.
- A single proof strategy covers hidden zeros across Yang-Mills, gravity, and the other theories.
Where Pith is reading between the lines
- Similar expansions, if available at loop level, could locate hidden zeros in higher-order amplitudes.
- Numerical verification of amplitude vanishing can be reduced to checking the simpler scalar case.
- The expansions may connect hidden zeros to other known amplitude identities such as color-kinematics relations.
- Specific low-point kinematic limits could be used to test whether additional hidden structures appear.
Load-bearing premise
The universal expansions are valid and complete for the kinematic configurations that produce the hidden zeros.
What would settle it
An explicit kinematic point where the bi-adjoint scalar amplitude vanishes but the corresponding Yang-Mills or gravitational amplitude remains non-zero, while the expansion is still applied.
read the original abstract
In this note, we derive and interpret hidden zeros of tree-level amplitudes of various theories, including Yang-Mills, non-linear sigma model, special Galileon, Dirac-Born-Infeld, and gravity, by utilizing universal expansions of tree-level amplitudes which expand amplitudes of different theories to those of bi-adjoint scalar theory. Hidden zeros of above amplitudes are attributed to zeros of bi-adjoint scalar amplitudes which can be easily proved. For unordered amplitudes such as gravitational ones, the kinematic condition for zeros causes potential divergences of propagators. We also show the detailed mechanism of eliminating such divergences.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that hidden zeros in tree-level amplitudes of Yang-Mills, non-linear sigma model, special Galileon, Dirac-Born-Infeld, and gravity theories follow directly from the zeros of bi-adjoint scalar (BAS) amplitudes via universal expansions that relate the different theories to BAS. It attributes the zeros to the easily proved BAS zeros and, for unordered amplitudes such as gravity, provides a mechanism showing how potential propagator divergences cancel under the relevant kinematic conditions.
Significance. If the expansions remain valid in the singular kinematic regime, the result supplies a unified and economical account of hidden zeros across several theories by reduction to the BAS case, without new parameters. The explicit treatment of divergence cancellation for gravitational amplitudes addresses a technical point that could otherwise obstruct application to unordered amplitudes. This strengthens the case for using BAS as a reference theory for amplitude properties.
major comments (2)
- The central claim requires that the universal expansions continue to hold when the chosen kinematic conditions render certain propagators on-shell (singular). The abstract states that divergences cancel, but this cancellation occurs after the expansion step and does not by itself establish that the expansion formulae themselves remain complete and valid in the singular limit. A concrete derivation or explicit check of the expansion under these conditions is needed to close the gap.
- The argument rests on the completeness of the cited universal expansions for the specific kinematic configurations that induce the zeros. If any derivation of those expansions assumed off-shell propagators or analytic continuation away from the mass shell, the reduction to BAS zeros would not automatically apply. The manuscript should identify the precise location where this applicability is verified.
Simulated Author's Rebuttal
We thank the referee for the careful reading and the constructive comments, which help clarify the scope of our claims. Below we respond point by point to the two major remarks.
read point-by-point responses
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Referee: The central claim requires that the universal expansions continue to hold when the chosen kinematic conditions render certain propagators on-shell (singular). The abstract states that divergences cancel, but this cancellation occurs after the expansion step and does not by itself establish that the expansion formulae themselves remain complete and valid in the singular limit. A concrete derivation or explicit check of the expansion under these conditions is needed to close the gap.
Authors: We agree that an explicit verification of the expansions inside the singular kinematic region strengthens the argument. The expansions themselves are algebraic identities obtained from the same set of Feynman rules that define the amplitudes; they therefore remain valid when a subset of propagators go on-shell. Nevertheless, to address the referee’s concern directly we will add a short subsection that performs the expansion explicitly for one representative theory (Yang-Mills) under the precise kinematic conditions that produce the hidden zero, confirming that no extra singular terms appear before the cancellation mechanism is applied. revision: yes
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Referee: The argument rests on the completeness of the cited universal expansions for the specific kinematic configurations that induce the zeros. If any derivation of those expansions assumed off-shell propagators or analytic continuation away from the mass shell, the reduction to BAS zeros would not automatically apply. The manuscript should identify the precise location where this applicability is verified.
Authors: The cited universal expansions are derived directly for on-shell tree amplitudes and do not invoke off-shell assumptions; their completeness follows from the same diagrammatic counting used for the ordinary amplitudes. The manuscript already applies them to the zero-inducing kinematics in Sections 3 and 4 and demonstrates consistency via the gravity cancellation. To make the verification explicit we will insert a clarifying sentence that points to the relevant equations and states that the expansions hold in the singular limit because they are identities among rational functions of the kinematic invariants. revision: yes
Circularity Check
No significant circularity; derivation relies on independent BAS zero proof
full rationale
The paper's chain uses cited universal expansions to map other amplitudes onto bi-adjoint scalar (BAS) amplitudes, then attributes the hidden zeros to BAS zeros that are described as independently and easily provable. The text also supplies an explicit mechanism for canceling propagator divergences under the chosen kinematics. No quoted step reduces a central prediction to a fitted parameter, self-definition, or load-bearing self-citation chain; the final attribution step stands on the separate BAS result rather than on the expansions alone. This is the normal non-circular case.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Universal expansions exist that express tree-level amplitudes of Yang-Mills, NLSM, sGal, DBI, and gravity in terms of bi-adjoint scalar amplitudes.
Forward citations
Cited by 7 Pith papers
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Universal Interpretation of Hidden Zero and $2$-Split of Tree-Level Amplitudes Using Feynman Diagrams, Part $\mathbf{I}$: ${\rm Tr}(\phi^3)$, NLSM and YM
A universal diagrammatic interpretation unifies hidden zeros (from massless on-shell conditions) and 2-splits (from double-line separation) in Tr(φ³), NLSM, and YM tree amplitudes using extended shuffle factorization ...
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Towards New Hidden Zero and $2$-Split of Loop-Level Feynman Integrands in ${\rm Tr}(\phi^3)$ Model
Loop-level hidden zeros and 2-split structures are found in Tr(φ³) Feynman integrands with simple kinematic conditions, generalizing the tree-level case to an L-loop integrand expressed as a sum over L+1 terms each wi...
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Hidden zeros for higher-derivative YM and GR amplitudes at tree-level
Hidden zeros extend to higher-derivative tree-level gluon and graviton amplitudes, with systematic cancellation of propagator singularities shown via bi-adjoint scalar expansions.
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A new recursion relation for tree-level NLSM amplitudes based on hidden zeros
A recursion for NLSM tree amplitudes based on hidden zeros reproduces the Adler zero, generates amplitudes from Tr(φ³) via δ-shift, expands them into bi-adjoint scalars, and claims these plus factorization uniquely de...
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Can Locality, Unitarity, and Hidden Zeros Completely Determine Tree-Level Amplitudes?
Locality, unitarity, and hidden zeros determine tree-level YM and NLSM amplitudes by reconstructing their soft theorems.
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$2$-split from Feynman diagrams and Expansions
Proof via Feynman diagrams that tree-level BAS⊕X amplitudes with X=YM,NLSM,GR obey 2-split under kinematic conditions, extended to pure X amplitudes with byproduct universal expansions of X currents into BAS currents.
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Soft theorems of tree-level ${\rm Tr}(\phi^3)$, YM and NLSM amplitudes from $2$-splits
Extends a 2-split factorization approach to reproduce known leading and sub-leading soft theorems for Tr(φ³) and YM single-soft and NLSM double-soft amplitudes while deriving higher-order universal forms and a kinemat...
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discussion (0)
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