Using a time dependent selfconsistent model for vertical sequential tunneling, we study the appearance of charge instabilities that lead to the formation of electric field domains in a weakly coupled doped superlattice in the presence of high magnetic fields parallel to the transport direction. The interplay between the high non linearity of the system -coming from the Coulomb interaction-and the inter-Landau-level scattering at the domain walls (regions of charge accumulation inside the superlattice) gives rise to new unstable negative differential conductance regions and extra stable branches in the sawtooth-like I-V curves.PACS numbers: 73.40. Gk, 72.15.Gd Weakly coupled doped semiconductor superlattices are an example of non linear systems in which all intrinsic properties related to high non linearity such as multistability, spatio-temporal chaos, etc, can be externally modified : e.g. by the application of a bias voltage or by the variation of the doping densities in the wells or in the contacts. The strong non linear transport that results from the Coulomb interaction in these systems presents a rich variety of new physical phenomena: multistability and electric field domains formation [1-3], self sustained oscillations [4], bifurcation to chaos [5], etc. In particular, the current flowing through a weakly coupled doped semiconductor superlattice presents a complicated sawtooth structure with unstable regions of negative differential conductance and multistable regions. This structure of branches comes from the charge instabilities that appear due to the motion of the domain wall (acummulation layer) from one well to another. This motion, which is due to resonant tunneling between adjacent subbands, leads to the formation of electric field domains. In this Letter we study theoretically for the first time this phenomenon in the presence of high magnetic fields parallel to the transport direction. New physical questions that were not relevant in the absence of magnetic fields can be raised. In particular, what happens to the charge instabilities in the presence of the new energy scale in the problem,hω c ? Resonant tunneling through double barriers [6-10] and superlattices [11] in the presence of high magnetic fields has been widely studied. Also, dynamical instabilities and bifurcations to chaos induced by a magnetic field in a double barrier resonant tunneling diode have been recently predicted [12]. It is well known that the application of a magnetic field perpendicular to a two dimensional electron gas produces the formation of Landau levels. For ideal samples, the tunneling through the heterostructure conserves the Landau level index. However, due to interface roughness, impurity scattering, or phonon scattering, these conservation rules are relaxed and inter Landau level transitions take place [6][7][8][9][10]. Recent magnetotransport experiments on weakly coupled doped semiconductor superlattices performed by Schmidt et al. [13] show new unstable regions of negative differential conductance and e...