State-of-the-art approaches to calculate the electron-phonon and the phonon-electron self-energy are based on a mean-field approximation for the interacting electronic system. This approach introduces an overscreening error which results in an underestimation of the electron-phonon coupling strength. We introduce a theoretical and numerical approach for the calculation of the phonon-electron self-energy without the overscreening error. Starting from the out-of-equilibrium Kadanoff-Baym equations for the phonon propagator, we discuss and compare the overscreened (i.e., symmetrically screened) and overscreening–free (i.e., asymmetrically screened) cases. We point out that the difficulty in treating the latter stems from the static approximation to the dielectric function and from the need to obtain a self-energy that preserves the elementary scattering processes. We solve both problems in the equilibrium case by considering a manifestly symmetric form of the correct self-energy which can be easily calculated numerically and yields an overscreening–free coupling strength. Finally, we describe the numerical implementation of this treatment into the first–principles Yambo code for the calculations of phonon linewidths.

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