jaxrts.hnc_potentials.SpinSeparatedEEExchange

class jaxrts.hnc_potentials.SpinSeparatedEEExchange

See [Wünsch et al., 2008], Eqn (17), Citing [Huang, 1987]. Eqn. (9.57), however, there is a factor of \(\sqrt{\pi}\) difference in the definition of lambda. (one is from [Deutsch, 1982] presenting a reduced quantity \(\lambda_{ee}\), and then them having another factor of \(\sqrt{2}\) in the mass term. We here present the corrected version of the equation, which reproduces Figure 6. in [Wünsch et al., 2008] and results in a higher repulsion than the SpinAveragedEEExchange, which should be expected.

Sets include_electrons to "SpinSeparated", automatically.

Methods

T(plasma_state)	The mass_weighted temperature average of a pair, according to [Schwarz et al., 2007].
__init__()	Sets include_electrons to "SpinSeparated", automatically.
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)	The Foutier transform of short_k().
long_r(plasma_state, r)	This is the long-range part of full_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)	The Fourier transform of short_r().
short_r(plasma_state, r)	This is the short-range part of full_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.SpinSeparatedEEExchange

HNC calculations with Quantum exchange potentials

HNC calculations with Quantum exchange potentials