Abstract

We calculate the low-lying glueball spectrum, several string tensions and some properties of topology and the running coupling for SU(N) lattice gauge theories in 3 + 1 dimensions. We do so for 2 ≤ N ≤ 12, using lattice simulations with the Wilson plaquette action, and for glueball states in all the representations of the cubic rotation group, for both values of parity and charge conjugation. We extrapolate these results to the continuum limit of each theory and then to N = ∞. For a number of these states we are able to identify their continuum spins with very little ambiguity. We calculate the fundamental string tension and k = 2 string tension and investigate the N dependence of the ratio. Using the string tension as the scale, we calculate the running of a lattice coupling and confirm that g2(a) ∝ 1/N for constant physics as N → ∞. We fit our calculated values of a√σ with the 3-loop β-function, and extract a value for {Lambda}_{overline{MS}} , in units of the string tension, for all our values of N, including SU(3). We use these fits to provide analytic formulae for estimating the string tension at a given lattice coupling. We calculate the topological charge Q for N ≤ 6 where it fluctuates sufficiently for a plausible estimate of the continuum topological susceptibility. We also calculate the renormalisation of the lattice topological charge, ZQ(β), for all our SU(N) gauge theories, using a standard definition of the charge, and we provide interpolating formulae, which may be useful in estimating the renormalisation of the lattice θ parameter. We provide quantitative results for how the topological charge ‘freezes’ with decreasing lattice spacing and with increasing N. Although we are able to show that within our typical errors our glueball and string tension results are insensitive to the freezing of Q at larger N and β, we choose to perform our calculations with a typical distribution of Q imposed upon the fields so as to further reduce any potential systematic errors.

Highlights

  • In this paper we calculate various physical properties of SU(N ) gauge theories in 3 + 1 dimensions

  • The loss of ergodicity with respect to the topological charge is illustrated for SU(8) in figure 22 where we show the values of QL after 2 and 20 cooling sweeps taken every 100 Monte Carlo sweeps for two sequences of 50000 sweeps generated at β = 47.75

  • Our primary goal in this paper has been to calculate the glueball spectra of a range of SU(N ) gauge theories, in the continuum limit, with enough precision to obtain plausible extrapolations to the theoretically interesting N = ∞ limit

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Summary

Introduction

In this paper we calculate various physical properties of SU(N ) gauge theories in 3 + 1 dimensions. In this paper we provide a calculation of the masses of the ground states and some excited states in all the irreducible representations R of the rotation group of our cubic lattice with an extrapolation of these masses (in units of the string tension) to the continuum limit. To make this extrapolation more reliable and more precise we extend the range of our calculations to much smaller lattice spacings than earlier work. We remark that in parallel with the present calculations most of our SU(3) calculations, which are of particular physical interest, have recently been published separately [11]

Lattice setup
Energies and correlators
Systematic errors
Topological freezing
String tensions
Finite volume corrections
Running coupling
Scaling with N
Perturbative running and ΛMS
Quantum numbers
Finite volume effects
Lattice masses
Strong-to-weak coupling transition
Continuum masses
Continuum spins
Scattering states
Some comparisons
Topological fluctuations
Topology and cooling
Tunneling between topological sectors
Topological susceptibility
Conclusions
A Lattice running couplings
N TrUp
Findings
B Scattering states
Full Text
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