Free Fermi and Bose Fields in TQFT and GBF
We present a rigorous and functorial quantization scheme for linear fermionic and bosonic field theory targeting the topological quantum field theory (TQFT) that is part of the general boundary formulation (GBF). Motivated by geometric quantization, we generalize a previous axiomatic characterizatio...
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National Academy of Science of Ukraine
2013-04-01
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doaj-6cab470825f24d9db0599a64ccab29a72020-11-24T22:26:44ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592013-04-019028Free Fermi and Bose Fields in TQFT and GBFRobert OecklWe present a rigorous and functorial quantization scheme for linear fermionic and bosonic field theory targeting the topological quantum field theory (TQFT) that is part of the general boundary formulation (GBF). Motivated by geometric quantization, we generalize a previous axiomatic characterization of classical linear bosonic field theory to include the fermionic case. We proceed to describe the quantization scheme, combining a Fock space quantization for state spaces with the Feynman path integral for amplitudes. We show rigorously that the resulting quantum theory satisfies the axioms of the TQFT, in a version generalized to include fermionic theories. In the bosonic case we show the equivalence to a previously developed holomorphic quantization scheme. Remarkably, it turns out that consistency in the fermionic case requires state spaces to be Krein spaces rather than Hilbert spaces. This is also supported by arguments from geometric quantization and by the explicit example of the Dirac field theory. Contrary to intuition from the standard formulation of quantum theory, we show that this is compatible with a consistent probability interpretation in the GBF. Another surprise in the fermionic case is the emergence of an algebraic notion of time, already in the classical theory, but inherited by the quantum theory. As in earlier work we need to impose an integrability condition in the bosonic case for all TQFT axioms to hold, due to the gluing anomaly. In contrast, we are able to renormalize this gluing anomaly in the fermionic case.http://dx.doi.org/10.3842/SIGMA.2013.028general boundary formulationtopological quantum field theoryfermionsfree field theoryfunctorial quantizationfoundations of quantum theoryquantum field theory |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Robert Oeckl |
spellingShingle |
Robert Oeckl Free Fermi and Bose Fields in TQFT and GBF Symmetry, Integrability and Geometry: Methods and Applications general boundary formulation topological quantum field theory fermions free field theory functorial quantization foundations of quantum theory quantum field theory |
author_facet |
Robert Oeckl |
author_sort |
Robert Oeckl |
title |
Free Fermi and Bose Fields in TQFT and GBF |
title_short |
Free Fermi and Bose Fields in TQFT and GBF |
title_full |
Free Fermi and Bose Fields in TQFT and GBF |
title_fullStr |
Free Fermi and Bose Fields in TQFT and GBF |
title_full_unstemmed |
Free Fermi and Bose Fields in TQFT and GBF |
title_sort |
free fermi and bose fields in tqft and gbf |
publisher |
National Academy of Science of Ukraine |
series |
Symmetry, Integrability and Geometry: Methods and Applications |
issn |
1815-0659 |
publishDate |
2013-04-01 |
description |
We present a rigorous and functorial quantization scheme for linear fermionic and bosonic field theory targeting the topological quantum field theory (TQFT) that is part of the general boundary formulation (GBF). Motivated by geometric quantization, we generalize a previous axiomatic characterization of classical linear bosonic field theory to include the fermionic case. We proceed to describe the quantization scheme, combining a Fock space quantization for state spaces with the Feynman path integral for amplitudes. We show rigorously that the resulting quantum theory satisfies the axioms of the TQFT, in a version generalized to include fermionic theories. In the bosonic case we show the equivalence to a previously developed holomorphic quantization scheme. Remarkably, it turns out that consistency in the fermionic case requires state spaces to be Krein spaces rather than Hilbert spaces. This is also supported by arguments from geometric quantization and by the explicit example of the Dirac field theory. Contrary to intuition from the standard formulation of quantum theory, we show that this is compatible with a consistent probability interpretation in the GBF. Another surprise in the fermionic case is the emergence of an algebraic notion of time, already in the classical theory, but inherited by the quantum theory. As in earlier work we need to impose an integrability condition in the bosonic case for all TQFT axioms to hold, due to the gluing anomaly. In contrast, we are able to renormalize this gluing anomaly in the fermionic case. |
topic |
general boundary formulation topological quantum field theory fermions free field theory functorial quantization foundations of quantum theory quantum field theory |
url |
http://dx.doi.org/10.3842/SIGMA.2013.028 |
work_keys_str_mv |
AT robertoeckl freefermiandbosefieldsintqftandgbf |
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