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Volumn 76, Issue 2, 2007, Pages

Collective and static properties of model two-component plasmas

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; DIELECTRIC PROPERTIES; ELECTRONS; MOLECULAR STRUCTURE; PROBABILITY; STATISTICAL MECHANICS;

EID: 34548154259     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.76.026403     Document Type: Article
Times cited : (20)

References (36)
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    • In non-hydrogen-like plasmas with polarizable ions, the first term on the right-hand side of Eqs. 5 11 should be substituted by the asymptotic value -1 (k,), i.e., by the value of -1 (k,ω) with ωp ω ωx, ωx being the characteristic excitation frequency of ions and, possibly, atoms. Then C0 (k) = -1 (k,) - -1 (k,0).
    • In non-hydrogen-like plasmas with polarizable ions, the first term on the right-hand side of Eqs. 5 11 should be substituted by the asymptotic value -1 (k,), i.e., by the value of -1 (k,ω) with ωp ω ωx, ωx being the characteristic excitation frequency of ions and, possibly, atoms. Then C0 (k) = -1 (k,) - -1 (k,0).
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    • This form of the Nevanlinna function follows from the Riesz-Herglotz integral representation 7 with dg (t) ∼ t dt.
    • This form of the Nevanlinna function follows from the Riesz-Herglotz integral representation 7 with dg (t) ∼ t dt.


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