2001
DOI: 10.1238/physica.regular.063a00219
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Spectrum and Energy Levels of Singly-Ionized Mercury (Hg II)

Abstract: The spectrum of singly-ionized mercury (Hg II) has been observed from 500 Ð to 9880 Ð with sliding sparks and pulsed-RF discharges on 10.7-m grating spectrographs in vacuum and air. About 500 lines have been classi¢ed as transitions between 114 energy levels. In addition to revising the existing system of 5d 10 nl, 5d 9 6s 2 , and 5d 9 6s6p energy levels, we have located new levels of the 5d 8 6s 2 6p, 5d 9 6s7p, 5d 9 6s5f, 5d 9 6s7s, 5d 9 6s6d, and 5d 9 6p 2 con-¢gurations, which occur in the region of the io… Show more

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Cited by 29 publications
(28 citation statements)
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References 31 publications
(61 reference statements)
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“…The wavelengths for the λ4358 and the λ3984 lines were taken from , while the oscillator strengths are experimental values adopted from Benck et al (1989) for Hg  λ4358 (log g f = +0.34) and Dworetsky (1980) for Hg  λ3984 (log g f = −1.73). Note should be made that the log g f value of the Hg  λ3984 line adopted here is 0.2 dex lower than the theoretically calculated values of Proffitt et al (1999) (log g f = −1.529) and Sansonetti & Reader (2001) (log g f = −1.51). In our investigation the experimentally determined g f value was chosen since its experimental nature allows for an uncertainty to be attached, while the theoretically calculated value is of indeterminable uncertainty.…”
Section: Abundance Analysis and Line Datacontrasting
confidence: 63%
“…The wavelengths for the λ4358 and the λ3984 lines were taken from , while the oscillator strengths are experimental values adopted from Benck et al (1989) for Hg  λ4358 (log g f = +0.34) and Dworetsky (1980) for Hg  λ3984 (log g f = −1.73). Note should be made that the log g f value of the Hg  λ3984 line adopted here is 0.2 dex lower than the theoretically calculated values of Proffitt et al (1999) (log g f = −1.529) and Sansonetti & Reader (2001) (log g f = −1.51). In our investigation the experimentally determined g f value was chosen since its experimental nature allows for an uncertainty to be attached, while the theoretically calculated value is of indeterminable uncertainty.…”
Section: Abundance Analysis and Line Datacontrasting
confidence: 63%
“…The spectral resolution of the spectra and the effect of rotational broadening prevent us from detecting the signature of hyperfine splitting. Mercury abundance was derived using the line of HgII at 398.39 nm with the oscillator strength from Sansonetti & Reader (2001).…”
Section: Input Datamentioning
confidence: 99%
“…The ionization energy of W + was found in Ref. [3] by means of the same method as here, using the scale factors for the 6s and 6p binding energies determined from the spectrum of Hg + analyzed by Sansonetti and Reader [22] and parametric fitting of the Hg 2+ levels from the ''Atomic Energy Levels'' compilation of C. Moore [23]. Another good reference point is provided by the analyses of Au + [24] and Au 2+ [25], where extensive and thorough parametric fitting was done and the IEs were accurately determined from high members of the Rydberg series.…”
Section: W 7+ (Ho-like) Through W 26+ (Cd-like)mentioning
confidence: 99%