SU(N) gauge theories in four dimensions: exploring the approach to N = infinity

We calculate the string tension, σ, and some of the lightest glueball masses, mG, in 3 + 1-dimensional SU(N) lattice gauge theories for 2 ≤ N ≤ 5. From the continuum extrapolation of the lattice values, we find that the mass ratios mG/√σ appear to show a rapid approach to the large-N limit, and, ind...

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Main Authors: Lucini, B, Teper, M
Format: Journal article
Published: 2001
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author Lucini, B
Teper, M
author_facet Lucini, B
Teper, M
author_sort Lucini, B
collection OXFORD
description We calculate the string tension, σ, and some of the lightest glueball masses, mG, in 3 + 1-dimensional SU(N) lattice gauge theories for 2 ≤ N ≤ 5. From the continuum extrapolation of the lattice values, we find that the mass ratios mG/√σ appear to show a rapid approach to the large-N limit, and, indeed, can be described all the way down to SU(2) using just a leading O(1/N2) correction. We confirm that the smooth large-N limit we find, is obtained by keeping a constant 't Hooft coupling. We also calculate the topological charge of the gauge fields. We observe that, as expected, the density of small-size instantons vanishes rapidly as N increases, while the topological susceptibility appears to have a non-zero N = ∞ limit.
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spelling oxford-uuid:aebb5654-e575-4a47-984e-25f4934b91b82022-03-27T03:44:31ZSU(N) gauge theories in four dimensions: exploring the approach to N = infinityJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:aebb5654-e575-4a47-984e-25f4934b91b8Symplectic Elements at Oxford2001Lucini, BTeper, MWe calculate the string tension, σ, and some of the lightest glueball masses, mG, in 3 + 1-dimensional SU(N) lattice gauge theories for 2 ≤ N ≤ 5. From the continuum extrapolation of the lattice values, we find that the mass ratios mG/√σ appear to show a rapid approach to the large-N limit, and, indeed, can be described all the way down to SU(2) using just a leading O(1/N2) correction. We confirm that the smooth large-N limit we find, is obtained by keeping a constant 't Hooft coupling. We also calculate the topological charge of the gauge fields. We observe that, as expected, the density of small-size instantons vanishes rapidly as N increases, while the topological susceptibility appears to have a non-zero N = ∞ limit.
spellingShingle Lucini, B
Teper, M
SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title_full SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title_fullStr SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title_full_unstemmed SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title_short SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
title_sort su n gauge theories in four dimensions exploring the approach to n infinity
work_keys_str_mv AT lucinib sungaugetheoriesinfourdimensionsexploringtheapproachtoninfinity
AT teperm sungaugetheoriesinfourdimensionsexploringtheapproachtoninfinity