Migdal's theorem in heavy fermion systems

The problem of non-adiabaticity in strongly correlated electron systems has been a subject of considerable attention. We concentrate on the role of vertex corrections to electron–phonon interaction for heavy fermion systems in the normal state. The range of energy transfer important for heavy fermio...

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Bibliographic Details
Published inPhysica. B, Condensed matter Vol. 259; pp. 498 - 500
Main Author Wojciechowski, R.J
Format Journal Article
LanguageEnglish
Published Elsevier B.V 1999
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Summary:The problem of non-adiabaticity in strongly correlated electron systems has been a subject of considerable attention. We concentrate on the role of vertex corrections to electron–phonon interaction for heavy fermion systems in the normal state. The range of energy transfer important for heavy fermion systems is not set by the energy characteristic of phonons (Debye energy), as in the case of normal metals, but is determined by the characteristic energy scale T ∗ (spin fluctuation temperature). To preserve characteristic features of heavy fermion systems we introduce a very simple model assuming a huge density of states near the Fermi level and a very large electron effective mass. We present an estimate of the lowest-order vertex correction to electron–phonon interaction and show that the Migdal's theorem is not valid for heavy fermion systems.
ISSN:0921-4526
1873-2135
DOI:10.1016/S0921-4526(98)00907-7