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Benjamin Buchholz

Publications and source records attributed to Benjamin Buchholz.

3 recordsLinked to original sources

Efficient calculation of the moments of runaway electron distribution functions

Plasma current instabilities can destabilize the plasma discharge and cool the plasma rapidly. In such $\textit{disruptions}$ or in the start-up phase of the reactor, inductive electric fields are generated which accelerate electrons to relativistic velocities, resulting in a beam of $\textit{runaway electrons}$. This can potentially damage the reactor vessel and must be avoided in future reactors such as ITER. Thus, the efficient simulation of the evolution of the runaway electron current is motivated for prediction, avoidance and attenuation of disruptions. In order to improve simulations based on a self-consistent calculation of the runaway electron current, the efficient computation of the moments of analytical runaway electron distribution functions is of interest. In this respect, the general procedure is carried out through the example of the distribution function of the $\textit{avalanche}$ generation of runaway electrons according to $\textit{F\"ul\"op et al.}$. At this the runaway electron number density, the current density and the mean mass-related kinetic energy density, which result from the zeroth, first and second moment are considered. Their analysis is carried out analytically and numerically. By means of a ${\rm M{\small ATLAB}}$ implementation, suitable calculation rules are derived and analyzed with regard to runtime efficiency. Finally, a physical evaluation of the components and the magnitude of the current density vector as well as the kinetic energy density for the plasma parameter space constructed from electric field, electron density and electron temperature is carried out, applying the derived efficient calculation rules. In addition, the applicability of the selected distribution function is discussed on the basis of graphical depictions of the results.

physics.plasm-ph

Calculation of the runaway electron current in tokamak disruptions

$\textit{Tokamak disruptions}$ can give rise to the $\textit{runaway phenomenon}$, which is typical in plasma physics and describes the almost unbound acceleration of electrons to relativistic velocities and can lead to the formation of a $\textit{runaway electron beam}$. In tokamak reactors like ITER, impacts of such a beam can damage the reactor wall, motivating the development of computationally efficient and accurate simulation methods for the runaway electron current. In present simulation software, the $\textit{reduced kinetic modeling}$ approach is used, which can be extended by using physically relevant moments of analytical runaway electron distribution functions. Because of this, calculation schemes for moments related to the density, the mean velocity and the mean kinetic energy of runaway electrons are deduced in this work and analysed with the help of ${\rm M{\small}{\small ATLAB}}$-implementations. At that, the screening effects of partially ionized impurities and different representations of the runaway electron generation region in momentum space are taken into account. First, numerical calculation rules for the primary $\textit{hot-tail}$ generation mechanism for isotropic and anisotropic two-dimensional descriptions of the runaway region are stated. They are then evaluated using the results of an ITER disruption simulation. After that, calculation concepts for said moments, related to the secondary $\textit{avalanche}$ generation mechanism, are derived. Different lower momentum boundaries for the runaway region and the influence of the partial screening of the nucleus by bound electrons are discussed on the basis of results calculated for different density combinations of a singly ionized deuterium-neon plasma. It is shown, that the analysed calculation schemes are physically valid and allow for the rapid investigation of physical quantities and parameter studies.

physics.plasm-ph

Evaluation of the $\textit{Breit-Hartree}$ contribution to the total energy of open atomic shells

In this work the $\textit{Breit-Hartree}$ interaction, as the lowest order relativistic correction to the $\textit{Coulomb}$ interaction, is extensively analyzed in the framework of relativistic $\textit{Density Functional Theory}$. Its relation to the magnetostatic dipole-dipole interaction is recapitulated, and its contribution to the total energy of the ground state of an atom or ion is investigated analytically and numerically. Specifically, an atom or ion is treated as a hollow sphere in zeroth order with a magnetization density solely generated by the spin density of open atomic shells. An analytical solution is derived for a radially dependent magnetization density within a spherical volume and implemented in ${\rm C}\texttt{++}$ and ${\rm M{\small}{\small ATLAB}}$. The $\textit{Breit-Hartree}$ contribution is calculated for an $\text{Mn}^{2+}$ and a $\text{Gd}^{3+}$ ion and compared with the second order $\textit{M}\hspace{-0.8mm}\require{cancel}\cancel{o}\hspace{-0.8mm}\textit{ller-Plesset}$ correlation energy correction. Additionally, the result for the $\text{Gd}^{3+}$ ion is discussed against the backdrop of experimental data and an improvement in experimental data prediction is shown. Moreover, the applicability of the $\textit{Breit-Hartree}$ contribution for atoms, ions and solid states is presented and a suggestion for further calculations of this correction for atoms and ions is submitted.

physics.chem-ph