SU(N) gauge theories in four dimensions: exploring the approach to N = infinity
By Biagio Lucini, M. Teper. 2001
197 citations recorded by the source corpus.
We calculate the string tension, K, and some of the lightest glueball masses, M, in 3+1 dimensional SU(N) lattice gauge theories for N=2,3,4,5 . From the continuum extrapolation of the lattice values, we find that the mass ratios, M/sqrt(K), 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/NxN) 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=infinity limit.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/925af55434c0eff27442dc1533b4070ed04df1b8
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In Nuclear and High Energy Physics
- E. Kiritsis
- Francesco Nitti
- U. Gursoy
- Georgios Michalogiorgakis
- L. Mazzanti
- U. Gürsoy
- Blaise Goutéraux
- Matti Järvinen
Citations in the corpus
- Thermal transport and drag force in improved holographic QCD (2009, background): “Although several lattice data are known at large-Nc, [65], others are not.”
- Improved holographic Yang–Mills at finite temperature: Comparison with data (2009, background): “HQCD Nc = 3 [28] Nc = ∞ [29] m0∗++/m0++ 1.”
- Improved Holographic QCD (2010, background): “The results for the parity-conserving sector are shown in Table 1, and are in good agreement with those reported by [61] for Nc = 3, whereas the results reported by [62] for large Nc are somewhat larger.”