We compute the low energy mass spectrum of lattice QCD in the large NC
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 NC, the masses of the low-lying
states in the unflavored meson spectrum. We then take the 't Hooft limit by
rescaling g2NC→g2; 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