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The strongly coupled phase of Yang-Mills plasma with arbitrary gauge groups is studied thanks to a T -matrix approach with the input of lattice-QCD static potentials. The existence of 2-gluon glueballs (considered here as 2-adjoint bound states) as well as the equation of state computed within the Dashen, Ma and Bernstein’s formalism are discussed. Results for SU(N) and G2 gauge groups are obtained and compared to current lattice data and G2 models.

Characterization of the pure-glue phase transition in QCD : Inclusion of the 2-body interactions thanks to the T-matrix formalism.