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The Stieltjes Bootstrap for Feynman Integrals

Abstract

We prove that scalar Feynman integrals are Stieltjes functions in each kinematic variable −pi· pj, as well as in the particle masses, for arbitrary loop order, arbitrary numbers of external legs, and arbitrary internal masses, whenever a certain exponent condition is satisfied. The proof rests on a canonical decomposition of the second Symanzik polynomial with manifestly non-negative coefficients indexed by spanning two-forests. We present a dedicated analysis of the case in which the kinematic variables satisfy relations, as frequently happens in physical applications. We argue that integration-by-parts relations allow the selection of master-integral bases in which every element is a Stieltjes function. The Stieltjes property guarantees the convergence of Padé approximants and provides determinantal (Hankel) constraints on the Taylor coefficients of master integrals that go beyond previously known complete-monotonicity bounds. We develop a numerical strategy that combines these Stieltjes constraints with differential equations to determine the master integrals in the Euclidean region via semidefinite optimization. We demonstrate this approach on the pedagogical example of the six-dimensional massive box integral, and then apply it to the calculation of previously unknown three-loop two-mass integrals needed for three-loop electroweak corrections to the Z- and Higgs-boson self-energies.

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BibTeX
@misc{brochet2026stieltjes,
  title = {{The Stieltjes Bootstrap for Feynman Integrals}},
  author = {Hadrien Brochet and Maximilian Haensch and Johannes Henn and Benjamin Hollering and Prashanth Raman and Qinglin Yang and Simone Zoia},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.37536},
  eprint = {2609.37536},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.37536},
}
RIS
TY  - UNPB
TI  - The Stieltjes Bootstrap for Feynman Integrals
AU  - Hadrien Brochet
AU  - Maximilian Haensch
AU  - Johannes Henn
AU  - Benjamin Hollering
AU  - Prashanth Raman
AU  - Qinglin Yang
AU  - Simone Zoia
PY  - 2026
DA  - 2026/09/29
PB  - arXiv
DO  - 10.48550/arxiv.2609.37536
UR  - https://arxiv.org/abs/2609.37536
AB  - We prove that scalar Feynman integrals are Stieltjes functions in each kinematic variable −p_i· p_j, as well as in the particle masses, for arbitrary loop order, arbitrary numbers of external legs, and arbitrary internal masses, whenever a certain exponent condition is satisfied. The proof rests on a canonical decomposition of the second Symanzik polynomial with manifestly non-negative coefficients indexed by spanning two-forests. We present a dedicated analysis of the case in which the kinematic variables satisfy relations, as frequently happens in physical applications. We argue that integration-by-parts relations allow the selection of master-integral bases in which every element is a Stieltjes function. The Stieltjes property guarantees the convergence of Padé approximants and provides determinantal (Hankel) constraints on the Taylor coefficients of master integrals that go beyond previously known complete-monotonicity bounds. We develop a numerical strategy that combines these Stieltjes constraints with differential equations to determine the master integrals in the Euclidean region via semidefinite optimization. We demonstrate this approach on the pedagogical example of the six-dimensional massive box integral, and then apply it to the calculation of previously unknown three-loop two-mass integrals needed for three-loop electroweak corrections to the Z- and Higgs-boson self-energies.
ER  -