  The famous peak-dip-hump lineshape of the (\pi,0) photoemission spectrum of
the bilayer Bi HTSC in the superconducting state is shown to be a superposition
of spectral features originating from different electronic states which reside
at different binding energies, but are each describable by essentially
identical single-particle spectral functions. The 'superconducting' peak is due
to the antibonding Cu-O-related band, while the hump is mainly formed by its
bonding counterpart, with a c-axis bilayer coupling induced splitting of about
140 meV.
