Cluster model

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Transition metals (ex. metallic Ni):

strongly-correlated d-band electrons

In Ni, the total bandwidth of 4s 3d valence electrons is of the order of 10eV.

The on-site electron-electron Coulomb repulsion obtained from Hartree-Fock or LDA atomic calculations is also of the order of 10eV.

For the solid, the state-of-the-art modified LDA and LSD calculations provide a quantitatively accurate description of the bandstructure, but fail in describing the multiplet splittings observed in core spectroscopies.

LDA
The Falicov 4-sites model, with periodic boundary conditions, accounts for the two points GAMMA and X of a fcc lattice bandstructure. Ni metal is represented in this model by 4 d shells at the 4 lattice sites, filled with 38 or 37 electrons (i.e. 2 or 3 holes). Atomic electron-electron correlations are treated exactly, and the bands are described at the two available points in terms of tight-binding integrals ddsigma, ddpi, dddelta.

Menchero has applied recently this Ni4 cluster model to the dichroism in core photoemission spectroscopy (XPS) [Phys. Rev. Lett. 76, 3208 (1996)], with apparently good results, but...

Dichroism in absorption

When we applied the same 4-sites model to the magnetic circular dichroism of Ni [Phys. Rev. B 42, 7262 (1996)], we found very poor agreement [or very good disagreement??] with experiment. In particular, such a basic property as the orbital angular momentum of the d electrons in the ground state is by far overestimated in the cluster model. Due to the well known sum rules [Phys. Rev. Lett. 76, 3208 (1996)], this implies a distorted dichroic signal. Furthermore, the amount of d8 configuration in the ground state admixture is by far underestimated in the origin model.

We tried to improve these properties changing the number of holes and tuning the bandstructure, getting closer to experimental observation. The final spectra are, however, in no better accord with experiment than what we could get out of a much simpler impurity model à la Anderson.

In the figure at the right, the lower part shows the isotropic and circular dichroic L2,3 x-ray absorption spectra (XAS) and the upper part gives the sum and the difference of the minority (up) and majority (down) 2p XPS spectra, in the same geometry as in the work by Menchero. Calculations are done for the Ni4 cluster with two X5 (dotted) and three X2 (solid) holes.

spectra of Ni

Those interested may read more in Manini, van Veenendaal, and Altarelli, Phys. Rev. Lett. 79, 2594 (1997).


created: 19 July 1999 last modified: 8 Jan 2026 by Nicola Manini