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− k2 hm2)((k0 + khp0)2 − (k1 + khp1)2) − k2 hm2) ⊂ P2 k × C3 while in three dimensions we have Y3D ⊂ P3 k × C4, similarly for higher dimensions

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hep-th 1

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2025 1

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CONDITIONAL 1

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Geometric Singularities of Feynman Integrals

hep-th · 2025-06-05 · conditional · novelty 6.0

A constructible function built from the vanishing hypersurface of a Feynman integrand is claimed to encode all Landau singularities, their microlocal directions, and the number of master integrals on each singular stratum.

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  • Geometric Singularities of Feynman Integrals hep-th · 2025-06-05 · conditional · none · ref 1

    A constructible function built from the vanishing hypersurface of a Feynman integrand is claimed to encode all Landau singularities, their microlocal directions, and the number of master integrals on each singular stratum.