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The Schrödinger functional: a renormalization probe for non-abelian gauge theories
Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
1992
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0550-3213(92)90466-O http://cds.cern.ch/record/234177 |
_version_ | 1780884473058951168 |
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author | Luscher, Martin Narayanan, Rajamani Weisz, Peter Wolff, Ulli |
author_facet | Luscher, Martin Narayanan, Rajamani Weisz, Peter Wolff, Ulli |
author_sort | Luscher, Martin |
collection | CERN |
description | Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schr\"odinger functional is carried through to 1-loop order. |
id | cern-234177 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1992 |
record_format | invenio |
spelling | cern-2341772023-10-04T06:48:30Zdoi:10.1016/0550-3213(92)90466-Ohttp://cds.cern.ch/record/234177engLuscher, MartinNarayanan, RajamaniWeisz, PeterWolff, UlliThe Schrödinger functional: a renormalization probe for non-abelian gauge theoriesGeneral Theoretical PhysicsFollowing Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schr\"odinger functional is carried through to 1-loop order.Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schr\"odinger functional is carried through to 1-loop order.Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schr\"odinger functional is carried through to 1-loop order.Following Symanzik we argue that the Schr\"odinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counter terms are required. The Schr\"odinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schr\"odinger functional is carried through to 1-loop order.Following Symanzik we argue that the Schrödinger functional in lattice gauge theories without matter fields has a well-defined continuum limit. Due to gauge invariance no extra counterterms are required. The Schrödinger functional is, moreover, accessible to numerical simulations. It may hence be used to study the scaling properties of the theory and in particular the evolution of the renormalized gauge coupling from low to high energies. A concrete proposition along this line is made and the necessary perturbative analysis of the Schrödinger functional is carried through to one-loop order.hep-lat/9207009DESY-92-025CERN-TH-6410-92CERN-TH-6410-92DESY-92-025oai:cds.cern.ch:2341771992 |
spellingShingle | General Theoretical Physics Luscher, Martin Narayanan, Rajamani Weisz, Peter Wolff, Ulli The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title | The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title_full | The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title_fullStr | The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title_full_unstemmed | The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title_short | The Schrödinger functional: a renormalization probe for non-abelian gauge theories |
title_sort | schrödinger functional: a renormalization probe for non-abelian gauge theories |
topic | General Theoretical Physics |
url | https://dx.doi.org/10.1016/0550-3213(92)90466-O http://cds.cern.ch/record/234177 |
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