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Some considerations on U eff values entering the hubbard hamiltonian
Author(s) -
Friedel J.,
Noguera C.
Publication year - 1983
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.560230411
Subject(s) - hamiltonian (control theory) , electron , hubbard model , physics , delocalized electron , quantum mechanics , atom (system on chip) , atomic physics , mathematics , superconductivity , mathematical optimization , computer science , embedded system
One of the simplest ways to take into account correlations between electrons in solid state physics, beyond the usual one electron approximation, is to use the Hubbard Hamiltonian\documentclass{article}\pagestyle{empty}\begin{document}$$\begin{array}{*{20}c} {H = \sum\limits_{ij} {\beta _{ij} C^\dag _{i\sigma } + U\sum\limits_i {n_{i\sigma } n(1 - \sigma )} } } & {n_i = C^\dag _i C_i }\\ \end{array} $$\end{document}Although it corresponds to very severe approximations, since intersite correlations are neglected, and since the whole problem is reduced to a single parameter U , it is already very difficult to solve, and exact solutions exist in only a few cases. It is thus not desired to introduce more complications in the Hamiltonian; but it could be interesting to understand, at least qualitatively, which processes influence the value taken by parameter U . The question arises in concrete cases, such as transition metals or organic molecules; comparing experiments and approximate solutions of the Hubbard Hamiltonian has shown that, in most cases, the value of U that yields the best fit is very different from what would be expected from atomic considerations. For instance, if one wants to study correlations on atoms of type M , a pure atomic point of view would affect to U the change in energy U at in the redox‐type equation\documentclass{article}\pagestyle{empty}\begin{document}$$ 2{\rm M} \mathbin{\lower.3ex\hbox{$\buildrel\textstyle\rightarrow\over{\smash{\leftarrow}\vphantom{_{\vbox to.5ex{\vss}}}}$}} {\rm M}^{\rm + } + {\rm M}^ - $$\end{document} . However it seems that solid state effects play an important role and we discuss, in this paper, three of them: (i) the finite time that one electron spends on a given atom due to the delocalization of the electrons in a band (effect of β ij which increases U relatively to U at ); (ii) the mixing of bands of different orbital character which allow two electrons not to be on the same orbital of an atom (and thus decreases U ); and (iii) the existence of Coulomb repulsion between electrons on neighboring sites which reduces their effective exclusion on the same site.

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