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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).
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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).
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34548157162
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This form of the Nevanlinna function follows from the Riesz-Herglotz integral representation 7 with dg (t) ∼ t dt.
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This form of the Nevanlinna function follows from the Riesz-Herglotz integral representation 7 with dg (t) ∼ t dt.
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