Abstract:We compute the wavelengths and oscillator strengths for the 3s, 3d → 2p, and 3p → 2s emission lines in Fe xix and Fe xx ions by using a configuration interaction Dirac-Fock and Dirac-Fock-Sturm method combined with second-order Brillouin-Wigner perturbation theory. We provide a complete list of computed wavelengths and oscillator strengths in both the velocity and length gauge for these transitions, many of which have never previously been reported. A comparison of our data with laboratory measurements and oth… Show more
“…The data sets of the n ≥ 3 states reported by Gu (2005bGu ( , 2007; Kotochigova et al (2007Kotochigova et al ( , 2010 are also of high accuracy. However, Gu (2005bGu ( , 2007 provided energy data for O-like Fe and Ni but not transition rates, and Kotochigova et al (2007Kotochigova et al ( , 2010 only reported transition wavelengths and rates in the range from 12 A to 16Å in Fe XIX.…”
Section: Introductionmentioning
confidence: 81%
“…Most of them targeted atomic data for low-lying states of the (1s 2 )2s 2 2p 4 , 2s2p 5 , and 2p 6 config-urations (the n = 2 complex) (Baluja & Zeippen 1988a,b;Galavis et al 1997;Vilkas et al 1999;Zhang & Sampson 2002;Gu 2005a;Hu et al 2011;Rynkun et al 2013;Fontes & Zhang 2015). Because of their wide applications for analyzing new observations of astrophysical sources, as well as for modeling and diagnosing a variety of plasmas, energy and transition data for higher-lying states of the n ≥ 3 complexes are also eagerly needed (Phillips et al 1982;Acton et al 1985;Landi & Phillips 2005;Kotochigova et al 2007Kotochigova et al , 2010Raassen & Pollock 2013). Among the studies of the n ≥ 3 states of Fe XIX we mention the calculations of Jonauskas et al (2004) using the multiconfiguration Dirac-Hartree-Fock (MCDHF) method, the calculations of Landi & Gu (2006) using the standard relativistic configuration interaction (RCI) method, the AUTOSTRUCTURE calculations of Butler & Badnell (2008), and the relativistic Breit-Pauli calculations of Nahar (2011).…”
Employing two state-of-the-art methods, multiconfiguration Dirac-Hartree-Fock and second-order many-body perturbation theory, the excitation energies and lifetimes for the lowest 200 states of the 2s 2 2p 4 , 2s2p 5 , 2p 6 , 2s 2 2p 3 3s, 2s 2 2p 3 3p, 2s 2 2p 3 3d, 2s2p 4 3s, 2s2p 4 3p, and 2s2p 4 3d configurations, and multipole (electric dipole (E1), magnetic dipole (M1), and electric quadrupole (E2)) transition rates, line strengths, and oscillator strengths among these states are calculated for each O-like ion from Cr XVII to Zn XXIII. Our two data sets are compared with the NIST and CHIANTI compiled values, and previous calculations. The data are accurate enough for identification and deblending of new emission lines from the sun and other astrophysical sources. The amount of data of high accuracy is significantly increased for the n = 3 states of several O-like ions of astrophysics interest, where experimental data are very scarce.
“…The data sets of the n ≥ 3 states reported by Gu (2005bGu ( , 2007; Kotochigova et al (2007Kotochigova et al ( , 2010 are also of high accuracy. However, Gu (2005bGu ( , 2007 provided energy data for O-like Fe and Ni but not transition rates, and Kotochigova et al (2007Kotochigova et al ( , 2010 only reported transition wavelengths and rates in the range from 12 A to 16Å in Fe XIX.…”
Section: Introductionmentioning
confidence: 81%
“…Most of them targeted atomic data for low-lying states of the (1s 2 )2s 2 2p 4 , 2s2p 5 , and 2p 6 config-urations (the n = 2 complex) (Baluja & Zeippen 1988a,b;Galavis et al 1997;Vilkas et al 1999;Zhang & Sampson 2002;Gu 2005a;Hu et al 2011;Rynkun et al 2013;Fontes & Zhang 2015). Because of their wide applications for analyzing new observations of astrophysical sources, as well as for modeling and diagnosing a variety of plasmas, energy and transition data for higher-lying states of the n ≥ 3 complexes are also eagerly needed (Phillips et al 1982;Acton et al 1985;Landi & Phillips 2005;Kotochigova et al 2007Kotochigova et al , 2010Raassen & Pollock 2013). Among the studies of the n ≥ 3 states of Fe XIX we mention the calculations of Jonauskas et al (2004) using the multiconfiguration Dirac-Hartree-Fock (MCDHF) method, the calculations of Landi & Gu (2006) using the standard relativistic configuration interaction (RCI) method, the AUTOSTRUCTURE calculations of Butler & Badnell (2008), and the relativistic Breit-Pauli calculations of Nahar (2011).…”
Employing two state-of-the-art methods, multiconfiguration Dirac-Hartree-Fock and second-order many-body perturbation theory, the excitation energies and lifetimes for the lowest 200 states of the 2s 2 2p 4 , 2s2p 5 , 2p 6 , 2s 2 2p 3 3s, 2s 2 2p 3 3p, 2s 2 2p 3 3d, 2s2p 4 3s, 2s2p 4 3p, and 2s2p 4 3d configurations, and multipole (electric dipole (E1), magnetic dipole (M1), and electric quadrupole (E2)) transition rates, line strengths, and oscillator strengths among these states are calculated for each O-like ion from Cr XVII to Zn XXIII. Our two data sets are compared with the NIST and CHIANTI compiled values, and previous calculations. The data are accurate enough for identification and deblending of new emission lines from the sun and other astrophysical sources. The amount of data of high accuracy is significantly increased for the n = 3 states of several O-like ions of astrophysics interest, where experimental data are very scarce.
“…A general observation is that the quartets states are energetically lower than the doublet states because electron correlation effects are smaller and converge faster with respect to the orbital set for high spin states than for low spin states Galvez et al 2005). The calculations Kotochigova et al (2010).…”
Section: Fe XXmentioning
confidence: 99%
“…, 30 were covered. Kotochigova et al (2010) evaluated the wavelengths and oscillator strengths for the 2s 2 2p 2 3s, 3d → 2s 2 2p 3 , and 2s2p 3 3p → 2s 2 2p 3 transitions in Fe XX using a configuration interaction Dirac-Fock-Sturm (MDFS) method combined with the second-order Brillouin-Wigner perturbation theory. Bhatia et al (1989) determined transition parameters between n = 2 and n = 3 levels of Ar XII, Ti XVI, Fe XX, Zn XXIV, and Kr XXX using the SUPERSTRUCTURE (SS) code.…”
Extensive multiconfiguration Dirac-Hartree-Fock (MCDHF) calculations and relativistic configuration interaction (RCI) calculations are performed for 272 states of the 2s 2 2p 3 , 2s2p 4 , 2p 5 , 2s 2 2p 2 3l, 2s2p 3 3l, and 2p 4 3l (l = 0, 1, 2) configurations in the nitrogen-like ions Cr XVIII, Fe XX, Ni XXII, and Zn XXIV. Valence, core-valence, and core-core electron correlation effects are accounted for through large configuration state function expansions. Calculated energy levels are compared with data from other calculations and with experimental data from the NIST database. Landé g J -factors; hyperfine structures; isotope shifts; and radiative electric dipole (E1), electric quadrupole (E2), and magnetic dipole (M1) transition rates are given for all ions. The accuracy of the calculated energy levels is high enough to facilitate identification of observed spectral lines involving the 2l 4 3l configurations, for which experimental data are largely missing.
“…A significant improvement in accuracy was achieved in the MBPT calculations compared with the results of the RCI method implemented in the FAC code, for example, uncertainties of wavelengths (Gu 2007) were determined to be a few mÅ through extensive comparison with the measurements of Chen et al (2007). The reliability and accuracy of this method were further confirmed by other elaborate theoretical calculations (Kotochigova et al 2007(Kotochigova et al , 2010Ekman et al 2014;Wang et al 2014) and very recent measurements (Gu et al 2011) in the EUV region. The present work has significantly increased the amount of available data for Be-like ions.…”
We report calculations of energy levels and radiative rates for transitions among the lowest 116 fine-structure levels arising from the ⩽ n 5 configurations in Be-like ions with Z = 10-30. The wavelengths, oscillator strengths, line strengths, and radiative rates for all possible electric dipole, magnetic dipole, electric quadrupole, and magnetic quadrupole transitions among the 116 levels have been calculated using the combined configuration interaction and many-body perturbation method. The accuracy of the results is determined through extensive comparisons with existing laboratory measurements and theoretical results. The present complete set of results should be of great help in line identification and the interpretation of spectra, as well as in the modeling and diagnostics of astrophysical and fusion plasmas.
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