2009
DOI: 10.1002/ctpp.200910011
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Electric Microfield Distributions in Li + Plasma With Account of the Ion Structure

Abstract: The electric microfield distributions at the location of an ion have been calculated using a coupling parameter integration technique for Li + plasma proposed by Ortner et al. [4] and Molecular Dynamics simulations. Electric microfield distributions are studied in a frame of the Hellmann-Gurskii-Krasko pseudopotential model, taking into account the quantum-mechanical effects and the ion shell structure [34]. The screened Hellmann-GurskiiKrasko pseudopotential taking into account not only the quantum-mecanical … Show more

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Cited by 10 publications
(42 citation statements)
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“…We will consider temperatures around 30000 K, where most of outer electrons are ionized, but the rest core electrons are still tightly bound. For the calculations of the EMD at a charged particle we need as an essential input quantity the pair distribution functions determined by the effective interactions of the plasma particles [1], [4]. In particular, the Deutsch [5] and the corrected Kelbg [6] potentials are frequently used.…”
Section: Introductionmentioning
confidence: 99%
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“…We will consider temperatures around 30000 K, where most of outer electrons are ionized, but the rest core electrons are still tightly bound. For the calculations of the EMD at a charged particle we need as an essential input quantity the pair distribution functions determined by the effective interactions of the plasma particles [1], [4]. In particular, the Deutsch [5] and the corrected Kelbg [6] potentials are frequently used.…”
Section: Introductionmentioning
confidence: 99%
“…High-temperatures alkali plasmas are widely applied in many technical projects [4]. For example, Li is an alkali metal of significant technological interest.…”
Section: Introductionmentioning
confidence: 99%
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“…A candidate for the coupling of the MD code is LAMMPS, which is capable of simulating a large scale molecular dynamics simulations, and it also could include particular interaction potential as well as all relevant processes of interest not included in the initial code as an additional module. The broadening parameters could be calculated from average energy and particle distributions and their temporal distributions, or, as an iterative procedure, a more real plasma potential could be obtained [20,21,28,29]. In the former case, the solutions would not necessary to be described as a set of analytical functions.…”
Section: The Calculated Quantitiesmentioning
confidence: 99%