We studied the influence of the electron-boson interaction (hybridization)
on the bosonic spectrum in the case of a two dimensional (2D) electronic sy
stem. The boson dispersion is affected by this interaction and we showed th
at for a constant density of states the wavevector dependence is quadratic
for qv(F)/4T much less than 1, and the imaginary part is small for qv(F)/4T
much greater than 1. However, the 2D electronic system presents a van Hove
density of states, and we considered this energy dependence in the calcula
tion of the bosonic energy spectrum. The real part becomes logarithmic depe
ndent on the wavevector and the imaginary part can be neglected if qv(F) si
milar to E-F or 2 E-c similar to z, for qv(F)/4T much greater than 1.