Abstract
We compute the spatial-volume dependence of the spectrum of 4D SU(3 ≤ N ≤ 6) gauge theories by lattice Monte-Carlo techniques. Setting the scale with the string tension, the spatial volume is L3 with 0.78fm ≤ L ≤ 2.3fm. The Euclidean `time' direction is kept large enough to be considered infinite and the boundary conditions are periodic in all four dimensions. We study the mixing of torelon pairs with the scalar and tensor glueballs, using a 2 × 2 Hamiltonian based on large-N counting rules. Looking to the other symmetry channels, finite-volume effects on the glueball spectrum are already surprisingly small in SU(3), and they become rapidly smaller as N is increased: several low-lying SU(6) states have no finite-volume corrections at the 1-2% level, at least down to L=0.9fm. We discuss the relation of this work with analytic calculations in small and intermediate volume, and with Eguchi-Kawai reduction in the planar limit.
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