Abstract
Recently, we (Es Sbihi Phil. Mag 2010) have successfully calculated, by molecular dynamics, the static structure factor of liquid bismuth at different temperatures. Our results were in very good agreement with the Waseda experimental data. Our assumption was to consider the true density of states which presents a gap as measured by Indlekofer (J. Non-Cryst. Solids 1989) and calculated by Hafner-Jank (Phys. Rev. B 1990) for liquid bismuth. The number of electrons at the Fermi energy has been calculated with three conduction electrons for bismuth (number of p electrons). With this assumption, the structures were determined with an effective ion-ion potential constructed from the Shaw local Optimised Model Potential (OMP) and the Ichimaru-Utsumi dielectric function. In the present paper, we generalize our assumptions to liquid thallium and lead which also present such a gap. Their calculated structures are also very close to the experimental ones. This confirms that the number of conduction electrons on the Fermi sphere is consistent with the number of p electrons as has been even shown for our electronic transport properties of liquid lead (A. Ben Abdellah, Phys. Rev. B 2003).
Highlights
The bismuth-lead alloy serves as cooling fluid in nuclear reactors [1]
This approach used in our previous work [3], was to consider the Density Of States (DOS) which presents a gap as measured by Indlekofer [4] and calculated by Hafner and Jank [5] for liquid bismuth
Our assumption confirms that the number of conduction electrons on the Fermi sphere is consistent with the number of p electrons as has been even shown for our electronic transport properties of liquid thallium and lead [10]
Summary
The bismuth-lead alloy serves as cooling fluid in nuclear reactors [1]. The knowledge of the physical properties of heavy metals is crucial for this technology [2]. In this paper we extend our new approach already used for bismuth [3] to others heavy metals as thallium and lead This approach used in our previous work [3], was to consider the Density Of States (DOS) which presents a gap as measured by Indlekofer [4] and calculated by Hafner and Jank [5] for liquid bismuth. The number of electrons at the Fermi energy has been calculated with three conduction electrons for bismuth (number of p electrons) With this assumption, the structures have been determined with an effective ion-ion potential constructed from the Shaw [6] local Optimised Model Potential (OMP) and the Ichimaru-Utsumi [7] dielectric function. We show the very good agreement between the experimental structure factors and the calculated ones for liquid thallium and lead with OMP and respectively one and two conduction electrons.
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