jaxrts.hnc_potentials.DeutschPotential

class jaxrts.hnc_potentials.DeutschPotential(include_electrons: Literal['off', 'SpinAveraged', 'SpinSeparated'] = 'off')[source]

Quantum diffraction potential suggested by C. Deutsch. See [Wünsch, 2011] Eqn. 4.43, who cites [Deutsch, 1977].

\[V_{a b}^{\mathrm{Deutsch}}(r) = \frac{q_{a}q_{b}}{4 \pi \varepsilon_0 r} \left[1-\exp\left(-\frac{r}{\lambda_{a b}}\right)\right]\]

Methods

`T`(plasma_state)	The mass_weighted temperature average of a pair, according to [Schwarz et al., 2007].
`__init__`([include_electrons])
`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 known Fourier transform of the Coulomb's potential long-range part.
`long_r`(plasma_state, r)	The long-range behavior of the Deutsch-Potentials should be the identical to the Coulomb-Potential.
`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)

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.DeutschPotential`