jaxrts.static_structure_factors.S_ii_AD

jaxrts.static_structure_factors.S_ii_AD(k: Quantity, T_e: Quantity, T_i: Quantity, n_e: Quantity, m_i: Quantity, Z_f: float) Quantity[source]

The static ion-ion structure factor, in the approach by Arkhipov and Davletov [Arkhipov and Davletov, 1998], as presented by [Gregori et al., 2003] in equation (7).

The method is using the Random Phase Approximation, treating the problem semi-classically and uses a pseudopotential between charged particles to account for quantum diffraction effects and symmetry.

Parameters:
  • k (Quantity) – The scattering vector length (units of 1/[length])

  • T_e (Quantity) – The electron temperature in Kelvin. Use T_cf_Greg() for the effective temperature used in [Gregori et al., 2003].

  • T_i (Quantity) – The ion temperature in Kelvin.

  • n_e (Quantity) – The electron density in 1/[volume]

  • m_i (Quantity) – The mass of the ion

  • Z_f (float) – Number of free electrons per ion.

Returns:

Quantity – Sii, the static ion ion structure factor.

Examples using jaxrts.static_structure_factors.S_ii_AD

Showing the relevance of the Born Mermin Approximation

Showing the relevance of the Born Mermin Approximation

Plot static structure Factors in the Approximation by Arkhipov and Devletov

Plot static structure Factors in the Approximation by Arkhipov and Devletov

Plot static structure factors in the Approximation by Gregori for T_i != T_e

Plot static structure factors in the Approximation by Gregori for T_i != T_e

Compare HNC Calculations to Gregori.2006

Compare HNC Calculations to Gregori.2006