One of the key requirements for good thermoelectric materials is a low lattice thermal conductivity. Here we present a combined neutron scattering and theoretical investigation of the lattice dynamics in the type I clathrate system Ba-Ge-Ni, which fulfills this requirement. We observe a strong hybridization between phonons of the Ba guest atoms and acoustic phonons of the Ge-Ni host structure over a wide region of the Brillouin zone which is in contrast with the frequently adopted picture of isolated Ba atoms in Ge-Ni host cages. It occurs without a strong decrease of the acoustic phonon lifetime which contradicts the usual assumption of strong anharmonic phononphonon scattering processes. Within the framework of ab-intio density functional theory calculations we interpret these hybridizations as a series of anti-crossings which act as a low pass filter, preventing the propagation of acoustic phonons. To highlight the effect of such a phononic low pass filter on the thermal transport, we compute the contribution of acoustic phonons to the thermal conductivity of Ba8Ge40Ni6 and compare it to those of pure Ge and a Ge46 empty-cage model system.A central issue in thermoelectrics research is to find materials that generate a high electromotive force under a small applied thermal gradient. The best thermoelectric materials (TE) should therefore combine a low lattice thermal conductivity with high electrical conductivity and thermopower. An efficient and economic way to reduce the thermal conductivity of bulk TE materials, without degrading their electronic properties, is to take advantage of inelastic resonant scattering between heatcarrying acoustic and non-propagative phonons, arising from isolated impurities with internal oscillator degrees of freedom. The librational vibration of molecules incorporated in crystal structures is a well-known example of such scattering centers and was formerly observed in KCl ionic crystals, doped with anionic molecules [1], or in the filled water nanocages of clathrate hydrates [2,3]. In TE clathrates and skutterudites, in which the phonon dispersions were recently investigated by means of inelastic neutrons scattering (INS) [4][5][6]10], the localized resonators are so-called rattling phonon modes of loosely bonded guest atoms in oversized atomic cages. The effect of inelastic resonant scattering [11,12] was described theoretically, using the relaxation-time approximation of the Boltzmann equation, in which the lattice thermal conductivity, κ L , for a cubic crystal can be expressed asHere C v (ω) is the phonon specific heat per unit volume and unit frequency, v(ω) is the mean group velocity for phonon frequency ω, τ (ω) is the mean time between collisions that destroy the heat current for all phonons of frequency ω and ρ 0 (ω) is the normalized vibrational density of states. The most common approach to evaluate the scattering of acoustic phonons by a resonator with frequency ω 0 is to add a phenomenological relaxation rate, τ −1where C is a constant proportional to the concentrat...