Recent progress in Hamiltonian light-front QCD
  Hamiltonian light-front quantum field theory constitutes a framework for the non-perturbative solution of invariant masses and correlated parton amplitudes of self-bound systems. By choosing light-front gauge and adopting a basis function representation, we obtain a large, sparse, Hamiltonian matrix for mass eigenstates of gauge theories that is solvable by adapting the ab initio no-core methods of nuclear many-body theory. Full covariance is recovered in the continuum limit, the infinite matrix limit. We outline our approach and discuss the computational challenges. 
J. P. Vary, H. Honkanen, Jun Li, P. Maris, S. J. Brodsky, P.   Sternberg, E. G. Ng, C. Yang