jaxrts.hnc_potentials.KlimontovichKraeftPotential.full_r
- KlimontovichKraeftPotential.full_r(plasma_state, r)[source]
- \[V_{e i}^{\mathrm{KK}}(r)=-\frac{k_{B}T\xi_{e i}^{2}}{16} \left[1+ \frac{4\pi\varepsilon_0 k_{B}T\xi_{e i}^{2}}{16Z e^{2}} r\right]^{-1}\]
In the above equation, \(\xi{e i} = (Z e^2 \beta) / (\lambda_{e i} 4 \pi \varepsilon_0)\).
\(Z e^{2} = q^2\), and \(\beta = 1/(k_B T)\) (see note above)
Examples using jaxrts.hnc_potentials.KlimontovichKraeftPotential.full_r
Static structure factor of the electron-ion system
Static structure factor of the electron-ion system