  The electron-doped cuprates were studied by electronic Raman spectroscopy
across the entire region of the superconducting (SC) phase diagram. We
determined that the magnitude of the SC order parameter varies between 4.6 and
3.5 k_BT_c, consistent with weak coupling BCS theory. Using a ``Raman
conductivity" sum rule, we found that doped carriers divide into coherent
quasi-particles (QPs) and carriers that remain incoherent. The coherent QPs
mainly reside in the vicinity of (pi/2a, pi/2a) regions of the Brillouin zone.
The carriers doped beyond optimal doping remain incoherent. Only coherent QPs
contribute to the superfluid density in the SC state.
