1974
DOI: 10.1016/0010-4655(74)90019-8
|View full text |Cite
|
Sign up to set email alerts
|

Techniques for the calculation of atomic structures and radiative data including relativistic corrections

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

9
580
0

Year Published

1994
1994
2016
2016

Publication Types

Select...
10

Relationship

0
10

Authors

Journals

citations
Cited by 953 publications
(589 citation statements)
references
References 44 publications
9
580
0
Order By: Relevance
“…(c) Since previous applications of FASTWIND have concentrated on O and early B stars, we briefly note that correct treatment of cooler stars requires sufficiently well described iron group ions of stages II/III, whose lines are dominating the background opacities for these objects. Details of the corresponding model atoms and line-lists (from superstructure, Eissner et al 1974;Nussbaumer & Storey 1978, augmented by data from Kurucz 1992) can be found in Pauldrach et al (2001). In order to rule out important effects from still missing data, we have constructed an alternative dataset which uses all Fe/Ni II/III lines from the Kurucz linelist.…”
Section: Determination Of Stellar and Wind Parametersmentioning
confidence: 99%
“…(c) Since previous applications of FASTWIND have concentrated on O and early B stars, we briefly note that correct treatment of cooler stars requires sufficiently well described iron group ions of stages II/III, whose lines are dominating the background opacities for these objects. Details of the corresponding model atoms and line-lists (from superstructure, Eissner et al 1974;Nussbaumer & Storey 1978, augmented by data from Kurucz 1992) can be found in Pauldrach et al (2001). In order to rule out important effects from still missing data, we have constructed an alternative dataset which uses all Fe/Ni II/III lines from the Kurucz linelist.…”
Section: Determination Of Stellar and Wind Parametersmentioning
confidence: 99%
“…The importance of accurate target representation in cc calculations is to be emphasized as the necessary first step. For the cc calculations for Fe II we obtain the target eigenfunctions for Fe III using the SUPERSTRUCTURE program by Eissner et al (1974) based on a scaled Thomas-Fermi-Dirac potential and configuration interaction (CI) wave-functions. Given the number of states needed in the calculations, the atomic structure calculations are rather complicated since proper account needs to be taken of the CI effects, while the total number of configurations must be kept small to minimize, as much as possible, the memory of the CPU requirements.…”
Section: Target Statesmentioning
confidence: 99%
“…Some of the discrepancies noted by Brickhouse et al and Young, Landi & Thomas (1998) were later resolved by Storey et al (2000), who also performed a large collisional calculation among the lowest 40 levels of the 3s 2 3p, 3s3p 2 , 3s 2 3d, 3p 3 and 3s3p3d configurations. For the determination of energy levels and radiative rates, they adopted the SuperStructure (SS) code of Eissner, Jones & Nussbaumer (1974), and for the scattering process the R-matrix code of Berrington et al (1978) was used. The calculations were basically performed in the LS coupling (Russell-Saunders or spin-orbit coupling), but mass and Darwin relativistic energy shifts were included through the term coupling coefficients while transforming the LS coupling reactance matrices to the intermediate coupling scheme.…”
Section: Introductionmentioning
confidence: 99%