This paper reports the use of a quantum theory of spectral line broadening and a realistic model potential to investigate non-adiabatic and inelastic excited state atomic collisions. The fully quantum mechanical lineshifts and widths are computed for the transition perturbed by Ar, using non-adiabatic theory. The effects of the j degeneracy and inelastic collisions for the transition are included and many validity tests are performed. Two-parameter pseudopotentials are used, for which , the radius about the Ar atom, and , the electron density (which is assumed constant within ) are adjustable. These parameters are varied to fit the computed shifts and widths to the experimental values over a range from 443 to 760 K. The contributions to the width and shift from the 7s state are larger than from the 4p state because of a shallow well in the 7s potential around 12.5 Å. The contribution of the non-adiabatic and inelastic terms to the width are small, although they increase with temperature and there are no inelastic contributions to the lineshift.