We show that the novel features observed in Raman experiments on optimally
doped and underdoped Bi-2212 compounds in B-1g geometry can be explained by
a strong fermionic self-energy due to the interaction with spin fluctuatio
ns. We compute the Raman intensity R(omega) both above and below T-c, and s
how that in both cases R(omega) progressively deviates, with decreasing dop
ing, from that in a Fermi-gas due to increasing contribution from the fermi
onic self-energy. We also show that the final state interaction increases w
ith decreasing doping and gradually transforms the 2 Delta peak in the supe
rconducting state into a pseudo resonance mode below 2 Delta. We argue that
these results agree well with the experimental data for Bi-2212. (C) 1999
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