Abstract

We compute the low energy mass spectrum of lattice QCD in the large NCN_C limit. Expanding around a gauge-invariant ground state, which spontaneously breaks the discrete chiral symmetry, we derive an improved strong-coupling expansion and evaluate, for any value of NCN_C, the masses of the low-lying states in the unflavored meson spectrum. We then take the 't Hooft limit by rescaling g2NCg2g^2 N_C\to g^2; the 't Hooft limit is smooth and no arbitrary parameters are needed. We find, already at the fourth order of the strong coupling perturbation theory, a very good agreement between the results of our lattice computation and the known continuum values.Comment: 43 pages, 1 figure. Minor corrections. One reference added in section

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    Last time updated on 03/01/2020