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A (Bounded) Bestiary of Feynman Integral Calabi-Yau Geometries

Jacob L. Bourjaily, Andrew J. McLeod, Matt von Hippel, Matthias Wilhelm

TL;DR

The paper introduces the concept of rigidity for Feynman integrals and proves a universal bound of $2(L-1)$ on the rigidity of massless four-dimensional integrals at $L$ loops, with maximal rigidity achieved by marginal graphs having $(L+1)D/2$ propagators. It shows that marginal integrals generically involve Calabi–Yau geometries whose dimension matches the integral's rigidity, providing explicit infinite families (tardigrades, paramecia, amoebas) and finite four-dimensional massless $\phi^4$ examples that saturate the bound. The analysis relies on the Symanzik polynomial formalism, where marginality corresponds to $\mathfrak{F}$ being linear in each Schwinger parameter, leading to integrals that can be viewed as weight-two polylogs over Calabi–Yau manifolds. The work discusses broader implications, conjectures extending the bound, and the relationship between geometry, planarity, and higher-loop structure, proposing a rich geometrical landscape beyond polylogarithms for loop integrals.

Abstract

We define the rigidity of a Feynman integral to be the smallest dimension over which it is non-polylogarithmic. We argue that massless Feynman integrals in four dimensions have a rigidity bounded by 2(L-1) at L loops, and we show that this bound may be saturated for integrals that we call marginal: those with (L+1)D/2 propagators in (even) D dimensions. We show that marginal Feynman integrals in D dimensions generically involve Calabi-Yau geometries, and we give examples of finite four-dimensional Feynman integrals in massless $φ^4$ theory that saturate our predicted bound in rigidity at all loop orders.

A (Bounded) Bestiary of Feynman Integral Calabi-Yau Geometries

TL;DR

The paper introduces the concept of rigidity for Feynman integrals and proves a universal bound of on the rigidity of massless four-dimensional integrals at loops, with maximal rigidity achieved by marginal graphs having propagators. It shows that marginal integrals generically involve Calabi–Yau geometries whose dimension matches the integral's rigidity, providing explicit infinite families (tardigrades, paramecia, amoebas) and finite four-dimensional massless examples that saturate the bound. The analysis relies on the Symanzik polynomial formalism, where marginality corresponds to being linear in each Schwinger parameter, leading to integrals that can be viewed as weight-two polylogs over Calabi–Yau manifolds. The work discusses broader implications, conjectures extending the bound, and the relationship between geometry, planarity, and higher-loop structure, proposing a rich geometrical landscape beyond polylogarithms for loop integrals.

Abstract

We define the rigidity of a Feynman integral to be the smallest dimension over which it is non-polylogarithmic. We argue that massless Feynman integrals in four dimensions have a rigidity bounded by 2(L-1) at L loops, and we show that this bound may be saturated for integrals that we call marginal: those with (L+1)D/2 propagators in (even) D dimensions. We show that marginal Feynman integrals in D dimensions generically involve Calabi-Yau geometries, and we give examples of finite four-dimensional Feynman integrals in massless theory that saturate our predicted bound in rigidity at all loop orders.

Paper Structure

This paper contains 2 sections, 2 equations.