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The bandshape of hydrogen bond vibrations in liquids is studied theoretically, taking into account the anharmonic coupling between the high-frequency stretching vibration, X−H→…Y (double well potential), and low-frequency lattice phonons, X←−H…Y→ (Morse potential), as well as Fermi resonances between states involving the X−H→…Y stretching and overtones or combinations of some internal modes. The relaxation of the fast mode (direct damping) and of the H-bond bridge (indirect damping) is incorporated by aid of previous results [N. Rekik, B.Ouari, P. Blaise, O. H. Rousseau, J. Mol. Struct. (Theochem) 687 (2004) 125–133]. The approach has been constructed in the framework of the linear response theory for which spectral density is obtained by Fourier transform of the autocorrelation function of the dipole moment operator of the fast mode. Numerical results show that mixing of all these effects results in …