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Status of Intersection Theory and Feynman Integrals

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arxiv 2002.10476 v2 pith:S7ENSMOT submitted 2020-02-24 hep-th hep-ph

classification hep-thhep-ph
keywords feynmanintegralsintersectiontheoryanalyticarticlecontributiondecember
verification ladder T0 review T1 audit T2 compute T3 formal

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We give a pedagogical review of the recently-introduced notion of a "scalar product" between Feynman integrals and how it helps us understand the analytic structure of the perturbative S-matrix. (This article is a contribution to the proceedings of the workshop "MathemAmplitudes 2019: Intersection Theory and Feynman Integrals" held in Padova, Italy on 18-20 December 2019.)

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Tame multi-leg Feynman integrals beyond one loop

    hep-ph 2024-12 reject novelty 7.0 of 10

    A 'branch' reformulation of Feynman integrals claims to reduce multi-loop integrals to one-loop-like low-dimensional integrals, but the advertised parameter bound is wrong and the numerical validation is not shown.

  2. Intersection matrices associated to geometric-ordered bases of Feynman integrals

    hep-th 2026-08 conditional novelty 6.0 of 10

    Intersection matrices of geometric-ordered Feynman integral bases are Laurent polynomials or, after a power-of-epsilon factor, integers, which enables systematic elimination of redundant auxiliary functions on the max...

  3. Differential Space of Feynman Integrals: Annihilators and $\mathcal{D}$-module

    hep-th 2025-06 conditional novelty 6.0 of 10

    A Griffiths-Dwork based algorithm builds annihilators and D-modules for Feynman-like integrals, and in all tested cases the holonomic rank matches the twisted de Rham cohomology dimension.

  4. Scaffolding Residues in Yang-Mills-Scalar \`a la CHY

    hep-th 2024-11 conditional novelty 6.0 of 10

    A CHY-level derivation showing that the scaffolding residue of 2n-scalar Yang-Mills-Scalar amplitudes reproduces n-gluon amplitudes, with the pfaffian of A turning into the pfaffian of Psi.

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