Partial and Total Dielectronic Recombination rate coefficients for W73+ to W56+

TL;DR

This paper provides detailed dielectronic recombination rate coefficients for tungsten ions W73+ to W56+, crucial for plasma modeling in fusion reactors, with improved accuracy and comprehensive data coverage.

Contribution

It presents the first partial and total DR rate coefficients for W73+ to W56+ using advanced atomic calculations, enhancing tungsten ionization balance models.

Findings

Rate coefficients agree within 20% with previous data for W63+ and W56+

Juttner correction significantly impacts tungsten ionization balance at high charge states

Data is available in standard formats for plasma modeling use

Abstract

Dielectronic recombination (DR) is a key atomic process which affects the spectroscopic diagnostic modelling of tungsten, most of whose ionization stages will be found somewhere in the ITER fusion reactor: in the edge, divertor, or core plasma. Accurate DR data is sparse while complete DR coverage is unsophisticated (e.g. average-atom or Burgess General Formula) as illustrated by the large uncertainties which currently exist in the tungsten ionization balance. To this end, we present a series of partial final state-resolved and total DR rate coefficients for W73+ to W56+ Tungsten ions. This is part of a wider effort within The Tungsten Project to calculate accurate dielectronic recombination rate coefficients for the tungsten isonuclear sequence for use in collisional-radiative modelling of finite-density tokamak plasmas. The recombination rate coefficients have been calculated with autostructure using kappa-averaged relativistic wavefunctions in level resolution (intermediate coupling) and configuration resolution (configuration average). The results are available from OPEN-ADAS according to the adf09 and adf48 standard formats. Comparison with previous calculations of total DR rate coefficients for W63+ and W56+ yield agreement to within 20% and 10%, respectively, at peak temperature. It is also seen that the Juttner correction to the Maxwell distribution has a significant effect on the ionization balance of tungsten at the highest charge states, changing both the peak abundance temperatures and the ionization fractions of several ions.