Abstract

Theoretical studies of tungsten ions in plasmas are presented. New calculations of the radiative recombination and photoionization cross-sections, as well as radiative recombination and radiated power loss rate coefficients have been performed for 54 tungsten ions for the range W6+–W71+. The data are of importance for fusion investigations at the reactor ITER, as well as devices ASDEX Upgrade and EBIT. Calculations are fully relativistic. Electron wave functions are found by the Dirac–Fock method with proper consideration of the electron exchange. All significant multipoles of the radiative field are taken into account. The radiative recombination rates and the radiated power loss rates are determined provided the continuum electron velocity is described by the relativistic Maxwell–Jüttner distribution. The impact of the core electron polarization on the radiative recombination cross-section is estimated for the Ne-like iron ion and for highly-charged tungsten ions within an analytical approximation using the Dirac–Fock electron wave functions. The effect is shown to enhance the radiative recombination cross-sections by ≲20%. The enhancement depends on the photon energy, the principal quantum number of polarized shells and the ion charge. The influence of plasma temperature and density on the electron structure of ions in local thermodynamic equilibrium plasmas is investigated. Results for the iron and uranium ions in dense plasmas are in good agreement with previous calculations. New calculations were performed for the tungsten ion in dense plasmas on the basis of the average-atom model, as well as for the impurity tungsten ion in fusion plasmas using the non-linear self-consistent field screening model. The temperature and density dependence of the ion charge, level energies and populations are considered.

Highlights

  • Experimental and theoretical investigation of tungsten becomes important due to its employment in up-to-date tokamaks

  • New calculations were performed for the tungsten ion in dense plasmas on the basis of the average-atom model, as well as for the impurity tungsten ion in fusion plasmas using the non-linear self-consistent field screening model

  • It is assumed that tungsten will be used as a plasma-facing material in the fusion reactor ITER due to such features as high thermal conductivity, a high melting point, low erosion, low sputtering and low tendency to trap tritium [1–3]

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Summary

Introduction

Experimental and theoretical investigation of tungsten becomes important due to its employment in up-to-date tokamaks. Calculations of the RR rates for these highly-charged tungsten ions, with the exception of W6+ , have been carried out in a wide temperature range [6]. The results were added to our extended unified database containing the RR and photoionization data for about 170 heavy element impurity ions occurring in fusion plasmas. The experimental values of the electron-impact excitation cross-section (EIECS) were determined in [13] by normalizing to measured intensities of the RR peaks, which were independently normalized to the associated theoretical RRCS. New results were obtained for the impurity tungsten ion in fusion plasmas at low temperatures using the non-linear self-consistent field screening model and for the dense tungsten plasmas in the wide temperature range using the average-atom model

Method of Calculations
Results and Discussion
Model Used in Calculations
PRR Effect for Fe XVII
PRR Effect for Highly-Charged Tungsten Ions
Average-Atom Model
Comparison with Previous Calculations
Results for Tungsten Ions
Conclusions
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