jaxrts.models
This submodule contains high-level wrappers for the different Models implemented.
Functions
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Create an average plasma state that shares the models of the original. |
Classes
A screening length valid for arbitrary degeneracy [Baggott, 2017]. |
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Model for the ion feature of the scattering, presented in [Arkhipov and Davletov, 1998] and [Arkhipov et al., 2000]. |
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This model performs a HNC calculation, assuming one average atom with a given, average charge state. |
These models implement potentials which can be when calculating the Born collision frequencies in |
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The Bohm-Staver relation for the Debye temperature, valid for 'simple metals', as it is presented in Eqn (3) of [Gregori et al., 2006a]. |
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Model for the free-free scattering, based on the Born Mermin Approximation ([Mermin, 1970]). |
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Model for the free-free scattering, based on the Born Mermin Approximation ([Mermin, 1970]). |
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Model for the free-free scattering, based on the Born Mermin Approximation ([Mermin, 1970]). |
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Model for the free-free scattering, based on the Born Mermin Approximation ([Mermin, 1970]). |
Model for the ion feature of the scattering, presented in [Gregori et al., 2007]. |
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A model that returns a constant chemical potential, specified by a user. |
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A model of constant Debye Temperature. |
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A model that returns a constant value for the IPD, set by the user. |
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A model that returns a constant screening length, given by a user. |
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Debye-Hückel IPD Model [Debye and Hückel, 1923]. |
Debye Hückel screening as presented by [Chapman et al., 2015]. |
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The standard Debye Hückel screening length. |
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A Debye Hückel potential, using the |
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This model approximates the static structure factor (SSF) of a solid at finite temperature as suggested by [Gregori et al., 2006a]. |
Chemical Potential of a fully degenerate electron gas, given by the Fermi energy. |
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Calculate the free-bound scattering by mirroring the free-bound scattering around the probing energy and applying a detailed balance factor to the intensity. |
Effective static approximation (ESA) of the local field correction model by Dornheim et al. [Dornheim et al., 2021]. |
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Ecker-Kröll IPD Model:[Ecker and Kröll, 1963]. |
Finite wavelength screening as presented by [Chapman et al., 2015], using a using a result from linear to calculate the screening density \(q\): |
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Uses finite wavelength screening to screen the bare Coulomb potential, i.e., \(V_{s}=\frac{V_\mathrm{Coulomb}}{\varepsilon_\text{RPA}(k, E=0)}\) |
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Model for the ion feature with a fixed value for \(S_{ii}\). |
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Form factor lowering model as introduced by [Döppner et al., 2023]. |
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A class of models suitable for |
The Debye-Hückel screening length. |
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Model for the ion feature of the scattering, presented in [Gregori et al., 2003]. |
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Calculating the screening from free electrons according to [Gregori et al., 2004]. |
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Model for the ion feature of the scattering, presented in [Gregori et al., 2006a]. |
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Screening model to calculate the screening charge q based on expression for the static structure factors given in [Gregori et al., 2007]. |
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A fitting formula for the chemical potential of an ideal electron gas between the classical and the quantum regime, given by [Gregori et al., 2003]. |
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Abstract class of `Model`s, describing the scattering by electrons tightly bound to the ions, causing quasi-elastic scattering. |
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Ion Sphere IPD Model [Rozsnyai, 1972]. |
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A constant local field correction which can be defined by the user. |
The screening density \(q\) is calculated using a result from linear response: |
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The screening density \(q\) is calculated using a result from linear response: |
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Abstract definition of a Model in jaxrts. |
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Universal model to neglect a contribution and set it to zero. |
Chemical Potential of a non-degenerate electron gas. |
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Calculates \(S_{ab}\) in the Hypernetted Chain approximation. |
Pauli Blocking IPD Model [Röpke et al., 2019]. |
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Analytical functions for each electrons in quantum states defined by the quantum numbers n and l, assuming a hydrogen-like atom. |
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A model for approximating \(S_\text{ii}\) as a sum of peaks. |
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Quantum Corrected Salpeter Approximation for free-free scattering. |
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Model for free-free scattering based on the Random Phase Approximation. |
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Model for free-free scattering based fitting to the Random Phase Approximation, as presented by [Dandrea et al., 1986]. |
Static local field correction model by Farid at al. |
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Static local field correction model by Geldart and Vosko [Geldart and Vosko, 1966]. |
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Static local field correction model that interpolates between the zero temperature result by Farid [Farid et al., 1993] and the Geldart result [Geldart and Vosko, 1966] for high temperatures. |
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Static local field correction model that interpolates between the zero temperature result by Utsumi and Ichimaru [Utsumi and Ichimaru, 1982] and the Geldart result [Geldart and Vosko, 1966] for high temperatures. |
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Static local field correction model by Utsumi and Ichimaru [Utsumi and Ichimaru, 1982]. |
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A subset of |
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Bound-free scattering based on the Schumacher Impulse Approximation [Schumacher et al., 1975]. |
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Bound-free scattering based on the Schumacher Impulse Approximation [Schumacher et al., 1975]. |
Bound-free scattering based on the Schumacher Impulse Approximation [Schumacher et al., 1975]. |
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Interpolation function between the low and high temperature limit for the chemical potential of a non-interacting (ideal) fermi gas given in the paper of Cowan [Cowan, 2019]. |
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Stewart Pyatt IPD Model [Stewart and Pyatt, 1966]. |
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Stewart Pyatt IPD Model [Stewart and Pyatt, 1966]. |
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This model sums up all \(S_{ab}\) from the HNC and multiplies it with \(\sqrt{x_{a}\cdot x_{b}}\). |
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Calculates \(S_{ab}\) including electron-ion and electron-electron static structure factors using the Hypernetted Chain approximation. |