  We address the issue whether ARPES measurements of the spectral function $A_k
(\omega)$ near the Fermi surface in the normal state of near optimally doped
cuprates can distinguish between the marginal Fermi liquid scenario and the
spin-fluctuation scenario. We argue that the data for momenta near the Fermi
surface are equally well described by both theories, but this agreement is
nearly meaningless as in both cases one has to add to $\Sigma^{\prime \prime}
(\omega)$ a large constant of yet unknown origin. We show that the data can be
well fitted by keeping only this constant term in the self-energy. To
distinguish between the two scenarios, one has to analyze the data away from
the Fermi surface, when the intrinsic piece in $\Sigma (\omega)$ becomes
dominant.
