An dynamical-mean-field-theory investigation of specific heat and electronic structure of $\alpha$ and $\delta$-plutonium

Abstract

We have carried out a comparative study of the electronic specific heat and electronic structure of $\alpha$ and $\delta$-plutonium using dynmical mean field theory (DMFT). We use the perturbative T-matrix and fluctuating exchange (T-matrix FLEX) as a quantum impurity solver. We considered two different physical pictures of plutonoium. In the first, $5f^5+$, the perturbative treatment of electronic correlations has been carried out around the non-magnetic (LDA) Hamiltonian, which results in an f occupation around a bit above $n_f=5$. In the second, $5f^6-$, plutonium is viewed as being close to an $5f^6$ configuration, and perturbation theory is carried out around the (LDA+U) starting point bit below $n_f=6$. In the latter case the electronic specific heat coefficient $\gamma$ attains a smaller value in $\gamma$-Pu than in $\alpha$-Pu, in contradiction to experiment, while in the former case our calculations reproduce the experimentally observed large increase of $\gamma$ in $\delta$-Pu as compared to the $\alpha$ phase. This enhancement of the electronic specific heat coefficient in $\delta$-Pu is due to strong electronic correlations present in this phase, which cause a substantial increase of the electronic effective mass, and high density of states at $E_F$. The densities of states of $\alpha$ and $\delta$-plutonium obtained starting from the open-shell configuration are also in good agreement with the experimental photoemission spectra.

6 pages, 3 figures

References in corpus (2)

• What is the valence of a correlated solid? The double life of delta-plutonium
• Magnetic state of plutonium ion in metallic Pu and its compounds

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