Feynman amplitudes on moduli spaces of graphs

This article introduces moduli spaces of coloured graphs on which Feynman amplitudes can be viewed as “discrete” volume densities. The basic idea behind this construction is that these moduli spaces decompose into disjoint unions of open cells on which parametric Feynman integrals are defined in a n...

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Main Author: Berghoff, M
Format: Journal article
Language:English
Published: European Mathematical Society Publishing House 2020
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author Berghoff, M
author_facet Berghoff, M
author_sort Berghoff, M
collection OXFORD
description This article introduces moduli spaces of coloured graphs on which Feynman amplitudes can be viewed as “discrete” volume densities. The basic idea behind this construction is that these moduli spaces decompose into disjoint unions of open cells on which parametric Feynman integrals are defined in a naturalway. Renormalisation of an amplitude translates then into the task of assigning to every cell a finite volume such that boundary relations between neighboring cells are respected. It is shown that this can be organized systematically using a type of Borel–Serre compactification of these moduli spaces. The key point is that in each compactified cell the newly added boundary components have a combinatorial description that resembles the forest structure of subdivergences of the corresponding Feynman diagram.
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spelling oxford-uuid:0b7d9b79-eb5d-449f-987a-d1beada12bbf2022-03-26T09:29:41ZFeynman amplitudes on moduli spaces of graphsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:0b7d9b79-eb5d-449f-987a-d1beada12bbfEnglishSymplectic ElementsEuropean Mathematical Society Publishing House2020Berghoff, MThis article introduces moduli spaces of coloured graphs on which Feynman amplitudes can be viewed as “discrete” volume densities. The basic idea behind this construction is that these moduli spaces decompose into disjoint unions of open cells on which parametric Feynman integrals are defined in a naturalway. Renormalisation of an amplitude translates then into the task of assigning to every cell a finite volume such that boundary relations between neighboring cells are respected. It is shown that this can be organized systematically using a type of Borel–Serre compactification of these moduli spaces. The key point is that in each compactified cell the newly added boundary components have a combinatorial description that resembles the forest structure of subdivergences of the corresponding Feynman diagram.
spellingShingle Berghoff, M
Feynman amplitudes on moduli spaces of graphs
title Feynman amplitudes on moduli spaces of graphs
title_full Feynman amplitudes on moduli spaces of graphs
title_fullStr Feynman amplitudes on moduli spaces of graphs
title_full_unstemmed Feynman amplitudes on moduli spaces of graphs
title_short Feynman amplitudes on moduli spaces of graphs
title_sort feynman amplitudes on moduli spaces of graphs
work_keys_str_mv AT berghoffm feynmanamplitudesonmodulispacesofgraphs