jaxrts.hnc_potentials.EmptyCorePotential

class jaxrts.hnc_potentials.EmptyCorePotential

The Empty core potential, which is essentially a CoulombPotential for all radii bigger than \(r_\text{cut}\). For all radii smaller than \(r_\text{cut}\), the potential is forced to zero.

We define \(r_\text{cut}\) in the jaxrts.PlasmaState.

Warning

This potential is only defined for the electron-ion interaction. Hence, it will always and automatically set ~:py:math:include_electrons to "SpinAveraged". For the rest, we return a Coulomb-potential – but this is really just to be compatible with the other potentials defined here.

Methods

T(plasma_state)	The mass_weighted temperature average of a pair, according to [Schwarz et al., 2007].
__init__()
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)
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_radius in the form required to be used with an :py:class:~.HNCPotential`.
short_k(plasma_state, k)
short_r(plasma_state, r)

Attributes

allowed_keys	A list of keys where this Potential is adequate for.
cite_keys	A list of bibtex keys.
include_electrons	If "SpinAveraged", the electrons are added as the n+1th ion species to the potential.

Examples using jaxrts.hnc_potentials.EmptyCorePotential

Electron ion potentials

Electron ion potentials