jaxrts.hnc_potentials.YukawaShortRangeRepulsion
- class jaxrts.hnc_potentials.YukawaShortRangeRepulsion(sigma: ~pint.registry.Quantity = <Quantity(0.0, 'angstrom')>)[source]
Yukawa Potential with a short-range repulsion as used in [Fletcher et al., 2015].
Methods
T(plasma_state)The mass_weighted temperature average of a pair, according to [Schwarz et al., 2007].
__init__([sigma])alpha(plasma_state)check(plasma_state)Test if the HNCPotential is applicable to the PlasmaState.
citation([style, comment])Return bibliographic information for the Model used.
full_k(plasma_state, k)full_r(plasma_state, r)kappa(plasma_state)lambda_ab(plasma_state)long_k(plasma_state, k)long_r(plasma_state, r)mu(plasma_state)The geometric mean of two masses (or reciprocal sum)
prepare(plasma_state, key)q2(plasma_state)This is \(q^2\)!
r_cut(plasma_state)This casts
jaxrts.PlasmaState.ion_core_radiusin the form required to be used with an :py:class:~.HNCPotential`.short_k(plasma_state, k)The Fourier transform of
short_r().short_r(plasma_state, r)Attributes
A list of keys where this Potential is adequate for.
A list of bibtex keys.
This gives the strength of the repulsion, and is a fitting parameter
If "SpinAveraged", the electrons are added as the n+1th ion species to the potential.