Isotope effects in the Hubbard-Holstein model within dynamical mean-field theory
arXiv:cond-mat/0609630 · doi:10.1103/PhysRevB.74.205108
Abstract
We study the isotope effects arising from the coupling of correlated electrons with dispersionless phonons by considering the Hubbard-Holstein model at half-filling within the dynamical mean-field theory. In particular we calculate the isotope effects on the quasi-particle spectral weight , the renormalized phonon frequency, and the static charge and spin susceptibilities. In the weakly correlated regime , where is the Hubbard repulsion and is the bare electron half-bandwidth, the physical properties are qualitatively similar to those characterizing the Holstein model in the absence of Coulomb repulsion, where the bipolaronic binding takes place at large electron-phonon coupling, and it reflects in divergent isotope responses. On the contrary in the strongly correlated regime , where the bipolaronic metal-insulator transition becomes of first order, the isotope effects are bounded, suggesting that the first order transition is likely driven by an electronic mechanism, rather then by a lattice instability. These results point out how the isotope responses are extremely sensitive to phase boundaries and they may be used to characterize the competition between the electron-phonon coupling and the Hubbard repulsion.
arXiv comment10 pages, 8 figures. The paper has been already accepted on Phys. Rev. B
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