We apply the time-dependent basis light-front quantization (tBLFQ) formalism, a Hamiltonian
approach which is suitable for non-perturbative problems to the deep inelastic scattering. We calculate the dipole cross section by explicitly evolving the quark-antiquark dipole in the field predicted by the Color Glass Condensate theory. Our formalism enables us to go
beyond Eikonal approximation and to include higher Fock sector contributions.
|Preferred Track||New Theoretical Developments|