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In E-DMFT, since the on-site interaction U does not get renormalized, one may find that the procedure of separating the Hartree contribution does not affect the result as far as the local interaction is concerned. So practically one can leave this term alone. The difference comes from the nonlocal interaction where the bare interaction vertex is replaced. by an effective, on-site, and retarded one.
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note
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The overall accuracy of E-DMFT, which consists of the QMC solution of the impurity model and the self-consistent calculations, is of the order 0.001. If not otherwise specified, all the data presented in this paper have an accuracy of ∼0.001. The centers of the various symbols in the diagrams represent the locations of the data while their sizes do not reflect the accuracy. All functions of the Matsubara frequency are calculated at the corresponding discrete values. The lines connecting the points are guides to the eye.
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In presenting the phonon-related results we always set λ = 0. A finite λ is used only in the QMC simulations.
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note
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We would like to thank Dr. S.S. Kancharla and Dr. C.J. Bolech for allowing us to use their DMRG programs for the calculation.
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