Abstract

We study shift relations between Feynman integrals via the Mellin transform through parametric annihilation operators. These contain the momentum space integration by parts relations, which are well known in the physics literature. Applying a result of Loeser and Sabbah, we conclude that the number of master integrals is computed by the Euler characteristic of the Lee–Pomeransky polynomial. We illustrate techniques to compute this Euler characteristic in various examples and compare it with numbers of master integrals obtained in previous works.

Highlights

  • At higher orders in perturbative quantum field theory, the computation of observables via Feynman diagrams involves a rapidly growing number of Feynman integrals

  • We recall that such parametric annihilators provide all shift relations between Feynman integrals, in particular the ones known from the classical integration by parts (IBP) method in momentum space

  • At first we fix conventions and notation for Feynman integrals in momentum space and recall their representations using Schwinger parameters. While the former is the setting for most traditional approaches to study IBP identities, it is the latter which provides the direct link to the theory of D-modules that our subsequent discussion will be based on

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Summary

Introduction

At higher orders in perturbative quantum field theory, the computation of observables via Feynman diagrams involves a rapidly growing number of Feynman integrals. In our set-up, these are differential operators P satisfying We recall that such parametric annihilators provide all shift relations between Feynman integrals, in particular the ones known from the classical IBP method in momentum space. We begin our article with a review of the momentum space and parametric representations of scalar Feynman integrals and recall how the Mellin transform translates shift relations to differential operators that annihilate the integrand. The relations between integrals in different dimensions are addressed, where we relate them to the Bernstein–Sato operators and show that these can be obtained from momentum space IBPs. Our main result is presented, where we apply the theory of Loeser and Sabbah to count the master integrals in terms of the Euler characteristic. “Appendix C” discusses the parametric annihilators of a two-loop example in detail

Feynman integrals and Schwinger parameters
Integral relations and the Mellin transform
Operator algebras and annihilators
On the correspondence to momentum space
Dimension shifts
Euler characteristic as number of master integrals
No master integrals
Graph polynomials
The Grothendieck ring of varieties
Tools and examples
Linearly reducible graphs
Sunrise graphs
General algorithms
Outlook
Integral representations
Momentum space and Schwinger parameters
Algebraic proof for Corollary 21
The Baikov representation
The theory of Loeser–Sabbah
43 Given a good filtration
A two-loop example
From annihilators to integral relations
Linear annihilators
From IBP relations to annihilators
Comparing annihilators and IBP operators
The number of master integrals
Full Text
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