On nonperturbative quantum field theory and noncommutative geometry

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OriginalspracheEnglisch
Aufsatznummer103466
Seitenumfang19
FachzeitschriftJournal of Geometry and Physics
Jahrgang145
Ausgabenummer145
Frühes Online-Datum28 Juni 2019
PublikationsstatusVeröffentlicht - Nov. 2019

Abstract

A general framework of non-perturbative quantum field theory on a curved background is proposed. A quantum field theory is in this setting characterised by an embedding of a space of field configurations into a Hilbert space over R . This embedding, which is only local up to a scale that we interpret as the Planck scale, coincides in the local and flat limit with the plane wave expansion known from canonical quantisation. We identify a universal Bott–Dirac operator acting in the Hilbert space over R and show that it gives rise to the free Hamiltonian both in the case of a scalar field theory and in the case of a Yang–Mills theory. These theories come with a canonical fermionic sector for which the Bott–Dirac operator also provides the Hamiltonian. We prove that Hilbert space representations of algebras of observables exist non-perturbatively for a real scalar theory and for a gauge theory, both with or without the fermionic sectors, and show that the free theories are given by semi-finite spectral triples over the respective configuration spaces. Finally, we propose a class of quantum field theories whose interactions are generated by inner fluctuations of the Bott–Dirac operator.

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On nonperturbative quantum field theory and noncommutative geometry. / Aastrup, Johannes; Grimstrup, Jesper M.
in: Journal of Geometry and Physics, Jahrgang 145, Nr. 145, 103466, 11.2019.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Aastrup J, Grimstrup JM. On nonperturbative quantum field theory and noncommutative geometry. Journal of Geometry and Physics. 2019 Nov;145(145):103466. Epub 2019 Jun 28. doi: 10.1016/j.geomphys.2019.06.017
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abstract = "A general framework of non-perturbative quantum field theory on a curved background is proposed. A quantum field theory is in this setting characterised by an embedding of a space of field configurations into a Hilbert space over R ∞. This embedding, which is only local up to a scale that we interpret as the Planck scale, coincides in the local and flat limit with the plane wave expansion known from canonical quantisation. We identify a universal Bott–Dirac operator acting in the Hilbert space over R ∞ and show that it gives rise to the free Hamiltonian both in the case of a scalar field theory and in the case of a Yang–Mills theory. These theories come with a canonical fermionic sector for which the Bott–Dirac operator also provides the Hamiltonian. We prove that Hilbert space representations of algebras of observables exist non-perturbatively for a real scalar theory and for a gauge theory, both with or without the fermionic sectors, and show that the free theories are given by semi-finite spectral triples over the respective configuration spaces. Finally, we propose a class of quantum field theories whose interactions are generated by inner fluctuations of the Bott–Dirac operator. ",
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