Stabilized spin-polarized jellium model and odd-even alternations in jellium metal clusters

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Abstract
In this paper, we have considered the mechanical stability of a jellium system in the presence of spin degrees of freedom and have generalized the stabilized jellium model, introduced by Perdew et al. [Phys. Rev. B 42, 11627 (1990)], to a spin-polarized case. By applying this generalization to metal clusters (Al, Ga, Li, Na, K, Cs), we gain additional insights about the odd-even alternations, seen in their ionization potentials. In this generalization, in addition to the electronic degrees of freedom, we allow the positive jellium background to expand as the clusters’ polarization increases. In fact, our self-consistent calculations of the energetics of alkali metal clusters with spherical geometries, in the context of density functional theory and local spin density approximation, show that the energy of a cluster is minimized for a configuration with maximum spin compensation (MSC). That is, for clusters with an even number of electrons, the energy minimization gives rise to complete compensation (N ↑ =N ↓ ), and for clusters with an odd number of electrons, only one electron remains uncompensated (N ↑ −N ↓ =1). It is this MSC rule which gives rise to alternations in the ionization potentials. Aside from very few exceptions, the MSC rule is also at work for other metal clusters (Al, Ga) of various sizes.