Recognition: unknown
On the Inverse Problem in Effective Field Theory
Pith reviewed 2026-05-10 09:53 UTC · model grok-4.3
The pith
The tree-level spectrum of heavy particles can be extracted directly from the Wilson coefficients of the low-energy effective field theory.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We show that the tree-level spectrum of heavy particles can be directly extracted from the Wilson coefficients of the corresponding effective field theory at low energies. This procedure is exact when the number of resonances is finite, and otherwise approximate. Our results are derived from a new class of analytic dispersion relations that depend nonlinearly on the scattering amplitude and apply to an exceedingly broad class of theories and kinematics.
What carries the argument
Nonlinear analytic dispersion relations that depend on the scattering amplitude and isolate the contributions of heavy particle poles from the low-energy Wilson coefficients.
If this is right
- The ultraviolet particle content can be reconstructed exactly from infrared Wilson coefficients when the number of resonances is finite.
- Approximate reconstruction of the spectrum remains possible for models with infinite towers of resonances.
- The extraction procedure applies across a wide range of scattering processes and effective theories without requiring a specific ultraviolet model.
- Low-energy measurements of Wilson coefficients can directly constrain the masses and couplings of heavy particles.
Where Pith is reading between the lines
- This inversion could allow direct fitting of ultraviolet parameters to experimental data on low-energy observables without intermediate model assumptions.
- The method might extend to cases with loop corrections if the dispersion relations can be generalized beyond tree level.
- It links the inverse problem in effective field theory to questions of analytic continuation and unitarity in broader quantum field theories.
Load-bearing premise
The scattering amplitude obeys the analytic properties required for the new nonlinear dispersion relations to hold, and the low-energy theory is accurately described at tree level with no significant loop corrections or non-analytic contributions.
What would settle it
An explicit computation in a known ultraviolet theory where the Wilson coefficients are matched to the low-energy theory and the dispersion relations then predict resonance masses or couplings that do not match the actual heavy spectrum.
Figures
read the original abstract
We show that the tree-level spectrum of heavy particles can be directly extracted from the Wilson coefficients of the corresponding effective field theory at low energies. This procedure is exact when the number of resonances is finite, and otherwise approximate. Our results are derived from a new class of analytic dispersion relations that depend nonlinearly on the scattering amplitude and apply to an exceedingly broad class of theories and kinematics.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that the tree-level spectrum of heavy particles (pole locations and residues) can be directly extracted from the Wilson coefficients of the low-energy effective field theory. This is achieved via a new class of nonlinear analytic dispersion relations that hold for a broad range of theories and kinematics. The extraction is asserted to be exact when the number of resonances is finite and approximate otherwise.
Significance. If the central derivation and inversion hold without hidden high-energy input or additional assumptions, the result would provide a direct, parameter-free link between IR EFT data and the UV resonance spectrum. This could be a useful tool for model-building and phenomenology in particle physics, as it avoids fitting procedures and relies only on analyticity properties of the amplitude.
major comments (2)
- [Abstract and §2] Abstract and §2: The claim of an 'exact' procedure for finite resonances requires an explicit demonstration that the nonlinear dispersion relations yield a unique, closed-form or algorithmic solution for the pole parameters solely from the Taylor coefficients (Wilson coefficients). Without a bijective map or concrete inversion formula shown, the step from the dispersion relation to spectrum extraction remains unverified and load-bearing for the main result.
- [§3.1, Eq. (8)] §3.1, Eq. (8): The nonlinear dispersion relation appears to involve a contour integral whose kernel may implicitly depend on the amplitude at scales above the EFT cutoff. Clarify whether this requires any UV input beyond the low-energy coefficients or if the nonlinearity is constructed to close entirely on the Taylor series.
minor comments (2)
- [Introduction] The notation distinguishing the full amplitude from its low-energy expansion could be introduced earlier and used consistently to avoid confusion in the derivation.
- [§4] A simple numerical example with a known finite-resonance model (e.g., two poles) should be added to illustrate the extraction procedure step-by-step.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments on our manuscript. We address the major comments point by point below, with clarifications on the derivation and indications of revisions to strengthen the presentation.
read point-by-point responses
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Referee: [Abstract and §2] Abstract and §2: The claim of an 'exact' procedure for finite resonances requires an explicit demonstration that the nonlinear dispersion relations yield a unique, closed-form or algorithmic solution for the pole parameters solely from the Taylor coefficients (Wilson coefficients). Without a bijective map or concrete inversion formula shown, the step from the dispersion relation to spectrum extraction remains unverified and load-bearing for the main result.
Authors: The manuscript derives the nonlinear dispersion relations in §2 and shows that, for a finite number of resonances, equating coefficients in the low-energy Taylor expansion produces a closed algebraic system whose solution yields the pole locations and residues uniquely. To make this inversion explicit and algorithmic, we will add a new subsection in the revised §2 containing a concrete procedure (including a matrix formulation for the general finite-resonance case) and a worked example for one resonance, demonstrating the direct map from Wilson coefficients to spectrum parameters. revision: yes
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Referee: [§3.1, Eq. (8)] §3.1, Eq. (8): The nonlinear dispersion relation appears to involve a contour integral whose kernel may implicitly depend on the amplitude at scales above the EFT cutoff. Clarify whether this requires any UV input beyond the low-energy coefficients or if the nonlinearity is constructed to close entirely on the Taylor series.
Authors: The nonlinearity in Eq. (8) is constructed precisely so that the contour integral closes on the low-energy Taylor series alone. High-energy contributions cancel identically due to the specific nonlinear combination of the amplitude, leaving an expression that depends only on the Wilson coefficients. We will revise §3.1 to include an explicit expansion showing this cancellation and confirming the absence of any UV input beyond the EFT data. revision: yes
Circularity Check
No significant circularity; derivation relies on new nonlinear dispersion relations applied to low-energy coefficients.
full rationale
The paper derives the extraction of heavy particle spectrum from Wilson coefficients using a new class of nonlinear analytic dispersion relations. No steps reduce the claimed inversion to a self-definition, fitted parameter renamed as prediction, or load-bearing self-citation. The procedure is presented as following from the dispersion relations applied to the low-energy Taylor expansion, without the output spectrum being defined in terms of the inputs by construction. The central claim has independent mathematical content from the new relations, and the abstract explicitly distinguishes exact (finite resonances) vs. approximate cases without smuggling assumptions via citation chains.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Scattering amplitudes are analytic in the complex energy plane except for physical cuts and poles
- domain assumption The low-energy theory is accurately captured at tree level
Forward citations
Cited by 1 Pith paper
-
Analytic Bootstrap of the Veneziano Amplitude
The Veneziano amplitude is the unique outcome of an analytic dual bootstrap from dispersive sum rules, unitarity, and either string monodromy or splitting and hidden-zero conditions.
Reference graph
Works this paper leans on
-
[1]
S.-L. Wan and S.-Y. Zhou, “Matrix moment approach to positivity bounds and UV reconstruction from IR,” JHEP02(2025) 168,arXiv:2411.11964 [hep-th]
-
[2]
N. Arkani-Hamed, T.-C. Huang, and Y.-t. Huang, “The EFT-Hedron,”JHEP05(2021) 259,arXiv:2012.15849 [hep-th]
-
[3]
B. Bellazzini, J. Elias Miró, R. Rattazzi, M. Riem- bau, and F. Riva, “Positive moments for scatter- ing amplitudes,”Phys. Rev. D104(2021) 036006, arXiv:2011.00037 [hep-th]
-
[4]
Schmüdgen,The Moment Problem
K. Schmüdgen,The Moment Problem. Graduate Texts in Mathematics. Springer International Publish- ing, 2017
2017
-
[5]
Note that this sum runs over all poles and zeros in the variablesin the amplitude. Such poles can even arise from long range force carriers in the EFT: for instance, massless exchanges in theschannel, which generate −1/s, or massless exchanges in thetchannel at fixed u, which generate1/(s+u)
-
[6]
[23] for an analogous construction of an amplitude-like object from the logarithmic derivative of the Landau-RiemannΞfunction, encoding the locations of the zeta function’s zeros
See Ref. [23] for an analogous construction of an amplitude-like object from the logarithmic derivative of the Landau-RiemannΞfunction, encoding the locations of the zeta function’s zeros
-
[7]
Cauchy’s argument principle states that 1 2πi ˛ γ f ′(z) f(z) dz=d zeros −d poles, wheref(z)is meromorphic andγis a closed curve en- circlingd zeros zeros andd poles poles off(z)
-
[8]
(10) by the de- gree of degeneracy
A higher-degree zero can be accommodated by allow- ingρto run over repeated elements or equivalently by rescaling the corresponding term in Eq. (10) by the de- gree of degeneracy. The same applies for poles, though higher-degree poles are forbidden by locality
-
[9]
Construction of a crossing-symmetric, Regge-behaved amplitude for linearly rising trajecto- ries,
G. Veneziano, “Construction of a crossing-symmetric, Regge-behaved amplitude for linearly rising trajecto- ries,”Nuovo Cim. A57(1968) 190
1968
-
[10]
Fork= 0and−1, this sum must of course be handled with care
-
[11]
S. Caron-Huot, Z. Komargodski, A. Sever, and A. Zhi- boedov, “Strings from Massive Higher Spins: The Asymptotic Uniqueness of the Veneziano Amplitude,” JHEP10(2017) 026,arXiv:1607.04253 [hep-th]
-
[12]
N. Arkani-Hamed, Q. Cao, J. Dong, C. Figueiredo, and S. He, “Hidden zeros for particle/string amplitudes and the unity of colored scalars, pions and gluons,”JHEP 10(2024) 231,arXiv:2312.16282 [hep-th]
-
[13]
O. Schlotterer and S. Stieberger, “Motivic Multiple Zeta Values and Superstring Amplitudes,”J. Phys. A46 (2013) 475401,arXiv:1205.1516 [hep-th]
-
[14]
Superstring amplitudes, uni- tarily, andHankeldeterminantsofmultiplezetavalues,
M. B. Green and C. Wen, “Superstring amplitudes, uni- tarily, andHankeldeterminantsofmultiplezetavalues,” JHEP11(2019) 079,arXiv:1908.08426 [hep-th]
-
[15]
In the case of higher-degree zeros, we keep theλn dis- tinct but absorb the degree of degeneracy into the mag- nitude ofσn. Meanwhile, if a pole and a zero happen to coincide, then their contributions cancel inck, the as- sociatedσn effectively vanishes, and the corresponding λn can be excluded from the sum. In such cases, the 6 Vandermonde matrix[λ]in =λ...
-
[16]
The convergence of Padé approximants of meromorphicfunctions,
J. Nuttall, “The convergence of Padé approximants of meromorphicfunctions,”Journal of Mathematical Anal- ysis and Applications31(1970) 147
1970
- [17]
-
[18]
ARelation Between Tree Amplitudes of Closed and Open Strings,
H.Kawai, D.C.Lewellen, andS.H.H.Tye, “ARelation Between Tree Amplitudes of Closed and Open Strings,” Nucl. Phys. B269(1986) 1
1986
-
[19]
Alternative Constructions of Crossing- Symmetric Amplitudes with Regge Behavior,
M. A. Virasoro, “Alternative Constructions of Crossing- Symmetric Amplitudes with Regge Behavior,”Phys. Rev.177(1969) 2309
1969
-
[20]
Electrostatic analogue for the Virasoro model,
J. A. Shapiro, “Electrostatic analogue for the Virasoro model,”Phys. Lett. B33(1970) 361
1970
-
[21]
Conformal Invariance of the One-Loop All-Plus Helicity Scattering Ampli- tudes,
J. Henn, B. Power, and S. Zoia, “Conformal Invariance of the One-Loop All-Plus Helicity Scattering Ampli- tudes,”JHEP02(2020) 019,arXiv:1911.12142 [hep-th]
-
[22]
One-loopn-point helicity amplitudes in (self- dual) gravity,
Z. Bern, L. J. Dixon, M. Perelstein, and J. S. Ro- zowsky, “One-loopn-point helicity amplitudes in (self- dual) gravity,”Phys. Lett. B444(1998) 273,arXiv:hep- th/9809160
-
[23]
Amplitudes and the Riemann Zeta Function,
G. N. Remmen, “Amplitudes and the Riemann Zeta Function,”Phys. Rev. Lett.127(2021) 241602, arXiv:2108.07820 [hep-th]
-
[24]
Ex- tractingresonancepolesfromnumericalscatteringdata: type-II Padé reconstruction,
D. Sokolovski, E. Akhmatskaya, and S. K. Sen, “Ex- tractingresonancepolesfromnumericalscatteringdata: type-II Padé reconstruction,”Comput. Phys. Commun. 182(2011) 448,arXiv:2204.05822 [physics.comp-ph]
-
[25]
Matrix methods for Padé approximation: Numerical calculation of poles, zeros and residues,
L. Perotti and M. Wojtylak, “Matrix methods for Padé approximation: Numerical calculation of poles, zeros and residues,”Linear Algebra and its Applications548 (2018) 95,1712.01155 [math.NA]. Appendix A: F romA(s)toQ(s).—The series ex- pansion ofQ(s) =dlogA(s)/dsencodes that exact same information as the series expansion forA(s). However, any experimental ...
discussion (0)
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