The nonadiabatic contribution of the electron-phonon interaction to th
e phonon self-energy Sigma(q, omega) of superconductors is studied for
different values of the phonon momentum q. It is demonstrated that th
e long range Coulomb field does not affect the nonadiabatic contributi
on of Sigma(q, co). It is shown in the framework of the BCS theory tha
t the vertex corrections for q = 0 lead to the appearance of the pole
in the phonon self-energy connected with the collective electron excit
ations inside the energy gap and can be an essential contribution to n
onadiabatic effects. Sigma(q, omega) has the logarithmic singularity n
ear omega approximate to 2 Delta for large values of q but the vertex
corrections are not important for this case. It is shown that for q =
Q, where Q is the nesting vector, the zero order phonon self-energy Si
gma(0)(Q, omega) has the square root singularity as well as for q = 0.
The vertex corrections lead again to the appearance of the pole in Si
gma(Q, omega) which has a strong influence on nonadiabatic effects. Th
e results are compared with the recent neutron scattering measurements
in borocarbides. (C) 1998 Published by Elsevier Science Ltd.