1972
DOI: 10.1002/pssb.2220510129
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Work Function and Surface Structure of Simple Metals

Abstract: The work function is calculated for ten simple metals in the framework of model potentials. The Shaw model potential is used. The surface structure is described b y a model containing a decrease of the conduction electron density and a change of the lattice constant. The parameters of this model are determined from the requirement of a minimum surface energy. The calculated work functions agree well with the experimental ones. The calculated increase of the lattice constant at the surface is about 1%. It gives… Show more

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Cited by 36 publications
(7 citation statements)
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“…The results of jellium-model-based calculations for twenty nontransition or simple polycrystalline metals by Heine and Hodges [42] and Paasch et al [43], yield generally lower values of the internal contribution, ranging between 3.7 eV for Pb or Hg and 0.8 eV for Al [42]. Comparison to the present values of A 1 for d transition metals, which range from 5.1 eV (Pt : FE) to 3.8 eV (Mo : FE), may be interesting in view of the different categories of metals.…”
Section: Results For "Average Surface"mentioning
confidence: 99%
“…The results of jellium-model-based calculations for twenty nontransition or simple polycrystalline metals by Heine and Hodges [42] and Paasch et al [43], yield generally lower values of the internal contribution, ranging between 3.7 eV for Pb or Hg and 0.8 eV for Al [42]. Comparison to the present values of A 1 for d transition metals, which range from 5.1 eV (Pt : FE) to 3.8 eV (Mo : FE), may be interesting in view of the different categories of metals.…”
Section: Results For "Average Surface"mentioning
confidence: 99%
“…Contrary to the calculation of Smith [3] and Sahni and Ma [7], all the energy functionals can be calculated analytically (including the surface correlation energy [22]) and expressed as functions of the parameter 8.…”
Section: 'mentioning
confidence: 99%
“…Initially we neglect the quantum mechanical reflection at the step potential. The current in the z direction is ~2 2e I (13) We assume the electron distribution function at equilibrium to be given stepwise in the two regions by f~~ i=1,2 (14) Then the current of electrons moving from left to right is given in the two regions by J~'-I k~o d3k kz, J~)-I k;'~ko d3k" k: (15) Ikl~kFa lk"l~ kF2…”
Section: Scattering By the Dipole Barriermentioning
confidence: 99%