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- M. Teper
- 1998

We calculate the mass spectra and string tensions of SU(2), SU(3), SU(4) and SU(5) gauge theories in 2+1 dimensions. We do so by simulating the corresponding lattice theories and then extrapolating… (More)

- Biagio Lucini, M. Teper, Urs Wenger
- 2005

We extend our earlier investigation of the finite temperature deconfinement transition in SU(N) gauge theories, with the emphasis on what happens as N??. We calculate the latent heat, Lh, in the… (More)

- Biagio Lucini, M. Teper
- 2001

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… (More)

We calculate the light `glueball' mass spectrum in N_f=2 lattice QCD using a fermion action that is non-perturbatively O(a) improved. We work at lattice spacings a ~0.1 fm and with quark masses that… (More)

- M. Teper
- 1998

We summarise what lattice simulations have to say about the physical properties of continuum SU(N) gauge theories in 3+1 dimensions. The quantities covered are: the glueball mass spectrum, the… (More)

Interpreting the way that the SU(3) bare lattice coupling runs with the lattice spacing is complicated by the fact that there is a smooth cross-over region in which the strong coupling expansion… (More)

- Biagio Lucini, M. Teper
- 2001

We calculate the string tensions of k-strings in $\mathrm{SU}(N)$ gauge theories in both 3 and 4 dimensions. We do so for SU(4) and SU(5) in $D=3+1,$ and for SU(4) and SU(6) in $D=2+1.$ In $D=3+1,$… (More)

- M. Teper
- 1985

Abstract After addressing the question of instanton stability on a space-time lattice, we investigate whether the full non-perturbative SU(2) gauge vacuum possesses an underlying (anti-)instanton… (More)

- M. Teper
- 1993

Abstract We perform finite temperature simulations of SU (2) lattice gauge fields in two spatial dimensions. We calculate the correlation length and find that it appears to diverge at a critical… (More)

- Francis Bursa, M. Teper
- 2006

We find a strong-to-weak coupling crossover in $D=2+1$ $SU(N)$ lattice gauge theories that appears to become a third-order phase transition at $N=\ensuremath{\infty}$, in a similar way to the… (More)