Taming non-analyticities of QFT observables

Abstract Many observables in quantum field theories are involved non-analytic functions of the parameters of the theory. However, it is expected that they are not arbitrarily wild, but rather have only a finite amount of geometric complexity. This expectation has been recently formalized by a tamene...

Full description

Saved in:
Bibliographic Details
Main Authors: Thomas W. Grimm, Giovanni Ravazzini, Mick van Vliet
Format: Article
Language:English
Published: SpringerOpen 2025-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP02(2025)009
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1823863414430105600
author Thomas W. Grimm
Giovanni Ravazzini
Mick van Vliet
author_facet Thomas W. Grimm
Giovanni Ravazzini
Mick van Vliet
author_sort Thomas W. Grimm
collection DOAJ
description Abstract Many observables in quantum field theories are involved non-analytic functions of the parameters of the theory. However, it is expected that they are not arbitrarily wild, but rather have only a finite amount of geometric complexity. This expectation has been recently formalized by a tameness principle: physical observables should be definable in o-minimal structures and their sharp refinements. In this work, we show that a broad class of non-analytic partition and correlation functions are tame functions in the o-minimal structure known as ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ — the structure defining Gevrey functions. Using a perturbative approach, we expand the observables in asymptotic series in powers of a small coupling constant. Although these series are often divergent, they can be Borel-resummed in the absence of Stokes phenomena to yield the full partition and correlation functions. We show that this makes them definable in ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ and provide a number of motivating examples. These include certain 0-dimensional quantum field theories and a set of higher-dimensional quantum field theories that can be analyzed using constructive field theory. Finally, we discuss how the eigenvalues of certain Hamiltonians in quantum mechanics are also definable in ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ .
format Article
id doaj-art-24290d84868443cf82dfde65ec59ae3b
institution Kabale University
issn 1029-8479
language English
publishDate 2025-02-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj-art-24290d84868443cf82dfde65ec59ae3b2025-02-09T12:08:41ZengSpringerOpenJournal of High Energy Physics1029-84792025-02-012025212810.1007/JHEP02(2025)009Taming non-analyticities of QFT observablesThomas W. Grimm0Giovanni Ravazzini1Mick van Vliet2Institute for Theoretical Physics, Utrecht UniversityInstitute for Theoretical Physics, Utrecht UniversityInstitute for Theoretical Physics, Utrecht UniversityAbstract Many observables in quantum field theories are involved non-analytic functions of the parameters of the theory. However, it is expected that they are not arbitrarily wild, but rather have only a finite amount of geometric complexity. This expectation has been recently formalized by a tameness principle: physical observables should be definable in o-minimal structures and their sharp refinements. In this work, we show that a broad class of non-analytic partition and correlation functions are tame functions in the o-minimal structure known as ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ — the structure defining Gevrey functions. Using a perturbative approach, we expand the observables in asymptotic series in powers of a small coupling constant. Although these series are often divergent, they can be Borel-resummed in the absence of Stokes phenomena to yield the full partition and correlation functions. We show that this makes them definable in ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ and provide a number of motivating examples. These include certain 0-dimensional quantum field theories and a set of higher-dimensional quantum field theories that can be analyzed using constructive field theory. Finally, we discuss how the eigenvalues of certain Hamiltonians in quantum mechanics are also definable in ℝ G $$ {\mathbb{R}}_{\mathcal{G}} $$ .https://doi.org/10.1007/JHEP02(2025)009Nonperturbative EffectsMatrix ModelsSolitons Monopoles and Instantons
spellingShingle Thomas W. Grimm
Giovanni Ravazzini
Mick van Vliet
Taming non-analyticities of QFT observables
Journal of High Energy Physics
Nonperturbative Effects
Matrix Models
Solitons Monopoles and Instantons
title Taming non-analyticities of QFT observables
title_full Taming non-analyticities of QFT observables
title_fullStr Taming non-analyticities of QFT observables
title_full_unstemmed Taming non-analyticities of QFT observables
title_short Taming non-analyticities of QFT observables
title_sort taming non analyticities of qft observables
topic Nonperturbative Effects
Matrix Models
Solitons Monopoles and Instantons
url https://doi.org/10.1007/JHEP02(2025)009
work_keys_str_mv AT thomaswgrimm tamingnonanalyticitiesofqftobservables
AT giovanniravazzini tamingnonanalyticitiesofqftobservables
AT mickvanvliet tamingnonanalyticitiesofqftobservables