Abstract

Heavy fermion systems show pronounced elastic anomalies at low temperatures below a characteristic temperature T * where quasi-particle bands are formed. To explain these anomalies a microscopic theory of electron–phonon interaction in heavy fermion systems is considered for the Periodic Anderson Model. The volume dependence of the hybridization between the f-electrons and the conduction electrons and of the bare f-electrons gives rise to the electron–phonon interaction. The phonon propagator, the phonon self-energy and the velocity of sound in the normal state are calculated at finite temperature and long wavelength limit of phonons. The effects of the phonon coupling strengths, f-level position and the hybridization on the anomalous temperature dependence of the velocity of sound are investigated. The results are discussed on the basis of the experimental results.

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